<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href="http://www.blogger.com/styles/atom.css" type="text/css"?><feed xmlns='http://www.w3.org/2005/Atom' xmlns:openSearch='http://a9.com/-/spec/opensearchrss/1.0/' xmlns:georss='http://www.georss.org/georss' xmlns:gd='http://schemas.google.com/g/2005' xmlns:thr='http://purl.org/syndication/thread/1.0'><id>tag:blogger.com,1999:blog-11580141</id><updated>2011-11-22T19:21:28.463-06:00</updated><category term='iMQC'/><category term='ddf'/><category term='nmr'/><category term='Science Daily'/><title type='text'>DDF and iMQC News</title><subtitle type='html'>News for the DDF and iMQC Research Community...

Please post news, comments, new papers, preprints...</subtitle><link rel='http://schemas.google.com/g/2005#feed' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/posts/default'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default?max-results=100'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/'/><link rel='hub' href='http://pubsubhubbub.appspot.com/'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><generator version='7.00' uri='http://www.blogger.com'>Blogger</generator><openSearch:totalResults>77</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>100</openSearch:itemsPerPage><entry><id>tag:blogger.com,1999:blog-11580141.post-7937842423092716660</id><published>2011-06-24T11:42:00.001-05:00</published><updated>2011-06-24T11:44:32.320-05:00</updated><title type='text'>Fast high-resolution 2D correlation spectroscopy in inhomogeneous fields via Hadamard intermolecular multiple quantum coherences technique</title><content type='html'>Congbo Cai, Fenglian Gao, Shuhui Cai, Yuqing Huang and Zhong Chen&lt;br /&gt;Journal of Magnetic Resonance&lt;br /&gt;Article in Press, Corrected Proof&lt;br /&gt;&lt;br /&gt;Recently, a method based on intermolecular multiple quantum coherences (iMQCs) has been proposed to obtain high-resolution 2D COSY spectra in inhomogeneous fields via 3D acquisitions. However, the very long acquisition time prevents its practical application. To overcome this shortage, the Hadamard technique was applied for the iMQC method in this paper. For the new pulse sequence, the direct frequency-domain excitation is used in the first indirect detection dimension, so the 3D acquisition was replaced by an array of 2D acquisitions. The acquisition time can be reduced to 10 min. The resulting spectra retain useful structural information including chemical shifts and multiplet patterns of J coupling even when the inhomogeneous line broadening leads to overlap of neighboring diagonal resonances in the conventional COSY spectrum. The experimental results are consistent with the theoretical predictions and computer simulations. The new sequence may provide a time-efficient way for the studies of chemical solution in inhomogeneous fields.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-7937842423092716660?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www.sciencedirect.com/science/article/pii/S1090780711001650' title='Fast high-resolution 2D correlation spectroscopy in inhomogeneous fields via Hadamard intermolecular multiple quantum coherences technique'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/7937842423092716660/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=7937842423092716660&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7937842423092716660'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7937842423092716660'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2011/06/fast-high-resolution-2d-correlation.html' title='Fast high-resolution 2D correlation spectroscopy in inhomogeneous fields via Hadamard intermolecular multiple quantum coherences technique'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4636884663859418025</id><published>2010-09-29T11:10:00.001-05:00</published><updated>2010-09-29T11:12:10.729-05:00</updated><title type='text'>Nearly 106-fold enhancements in intermolecular 1H double-quantum NMR experiments by nuclear hyperpolarization</title><content type='html'>Mor Mishkovsky, Uzi Eliav, Gil Navon and Lucio Frydman&lt;br /&gt;Journal of Magnetic Resonance&lt;br /&gt;Volume 200, Issue 1, September 2009, Pages 142-146 &lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;&lt;br /&gt;Intermolecular Multiple-Quantum Coherences (iMQCs) can yield interesting NMR information of high potential usefulness in spectroscopy and imaging – provided their associated sensitivity limitations can be overcome. A recent study demonstrated that ex situ dynamic nuclear polarization (DNP) could assist in overcoming sensitivity problems for iMQC-based experiments on 13C nuclei. In the present work we show that a similar approach is possible when targeting the protons of a hyperpolarized solvent. It was found that although the DNP procedure enhances single-quantum 1H signals by about 600, which is significantly less than in optimized low-γ  liquid-state counterparts, the non-linear dependence of iMQC-derived signals on polarization can yield very large enhancements approaching 106. Cleary no practical amount of data averaging can match this kind of sensitivity gains. The fact that DNP endows iMQC-based 1H NMR spectra with a sensitivity that amply exceeds that of their thermally polarized single-quantum counterpart, is confirmed in a number of simple single-scan 2D imaging experiments.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4636884663859418025?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2009.06.002' title='Nearly 106-fold enhancements in intermolecular 1H double-quantum NMR experiments by nuclear hyperpolarization'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4636884663859418025/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4636884663859418025&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4636884663859418025'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4636884663859418025'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2010/09/nearly-106-fold-enhancements-in.html' title='Nearly 106-fold enhancements in intermolecular 1H double-quantum NMR experiments by nuclear hyperpolarization'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-2075765123829615707</id><published>2010-09-29T11:06:00.001-05:00</published><updated>2010-09-29T11:08:27.827-05:00</updated><title type='text'>Intermolecular single-quantum coherence sequences for high-resolution NMR spectra in inhomogeneous fields</title><content type='html'>Yuqing Huang, Shuhui Cai, Xi Chen and Zhong Chen&lt;br /&gt;Journal of Magnetic Resonance&lt;br /&gt;Volume 203, Issue 1, March 2010, Pages 100-107 &lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;&lt;br /&gt;A new pulse sequence based on intermolecular single-quantum coherences (iSQCs) is proposed to obtain high-resolution NMR spectroscopy in inhomogeneous magnetic fields via fast 2D acquisition. Taking the intrinsic properties of iSQCs, the sequence is time-efficient with a narrow spectral width in the indirect dimension. It can recover useful information of chemical shifts, relative peak areas, J coupling constants, and multiplet patterns even when the field inhomogeneity is severe enough to erase almost all spectroscopic information. Moreover, good solvent suppression efficiency can be achieved by this sequence even with imperfect radio-frequency pulse flip angles. Spatially localized iSQC spectroscopy was performed on a sample packed with pig brain tissue and cucumber to show the feasibility of the sequence in in vivo magnetic resonance spectroscopy (MRS). This sequence may provide a promising way for the applications on in vivo and in situ high-resolution NMR spectroscopy.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-2075765123829615707?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2009.12.007' title='Intermolecular single-quantum coherence sequences for high-resolution NMR spectra in inhomogeneous fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/2075765123829615707/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=2075765123829615707&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2075765123829615707'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2075765123829615707'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2010/09/intermolecular-single-quantum-coherence.html' title='Intermolecular single-quantum coherence sequences for high-resolution NMR spectra in inhomogeneous fields'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1040305747843880615</id><published>2010-05-25T14:25:00.000-05:00</published><updated>2010-05-25T14:28:33.974-05:00</updated><title type='text'>Highly efficient square wave distant dipolar field and its application for in vivo MRI</title><content type='html'>Congbo Cai, Fenglian Gao , Shuhui Cai, Jianhui Zhong, Zhong Chen&lt;br /&gt;&lt;br /&gt;Intermolecular multiple quantum coherences generated by distant dipolar field (DDF) have some attractive properties, but the intrinsic weak signal intensity prevents their widespread applications. Recently, Branca et al. (J Chem Phys 2008;129:054502) suggested that square wave DDF was more efficient than conventional sinusoidal DDF because it could simultaneously produce intermolecular multiple quantum coherences signal with various major orders. In this article, instead of a series of adiabatic inversion pulses proposed previously, a more efficient composite adiabatic inversion pulse was applied to create square wave DDF. The square wave DDF was applied to in vivo MRI for the first time, and the corresponding simulations were performed. Both experimental and simulated results show that square wave DDF with composite adiabatic inversion pulse improves over the original Z-modulation enhanced to binary for self-refocused acquisition implementation and can enhance the signal intensity to about 2-fold of that from conventional correlation spectroscopy (COSY) revamped with asymmetric Z-gradient echo detection sequence for in vivo MRI, close to the theoretical prediction. Magn Reson Med, 2010. © 2010 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1040305747843880615?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www3.interscience.wiley.com/journal/123416074/abstract' title='Highly efficient square wave distant dipolar field and its application for in vivo MRI'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1040305747843880615/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1040305747843880615&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1040305747843880615'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1040305747843880615'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2010/05/highly-efficient-square-wave-distant.html' title='Highly efficient square wave distant dipolar field and its application for in vivo MRI'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-2242293384859030748</id><published>2009-03-25T17:16:00.001-05:00</published><updated>2009-03-25T17:18:03.159-05:00</updated><title type='text'>Fast acquisition scheme for achieving high-resolution MRS with J-scaling under inhomogeneous fields</title><content type='html'>Xi Chen, Meijin Lin, Zhong Chen, and Jianhui Zhong&lt;br /&gt;Magnetic Resonance in Medicine&lt;br /&gt;Volume 61 Issue 4, Pages 775 - 784&lt;br /&gt;Published Online: 2 Feb 2009&lt;br /&gt;&lt;br /&gt;Intermolecular multiple-quantum coherences (iMQCs) can refocus the phase dispersion caused by magnetic field inhomogeneities while preserving the chemical shift, so they have been applied to achieve high-resolution MR spectroscopy free of line broadening caused by susceptibility gradients. However, previous iMQC high-resolution methods all require two-dimensional spectra sampling of the full range of chemical shifts of solute evolutions in both F1 and F2 dimensions, resulting in a prolonged scanning time for data acquisition. In this work, sparse sampling in the t1 dimension and subsequent fold-over correction are used to speed up the intermolecular zero-quantum coherence spectroscopy by up to 50 times on high-field MR systems. Furthermore, three types of spectra with homo-decoupling, original J-coupling constants, and doubled J-coupling constants respectively are obtained with manipulation of the t1 period. The water suppression is also improved by the combined use of intermolecular double-quantum filter and excitation sculpting. The feasibilities of this group of new sequences are demonstrated by experiments using an agar gel phantom with an air bubble, in vitro pig brain tissues and an intact postmortem mudskipper. Magn Reson Med, 2009. © 2009 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-2242293384859030748?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21894' title='Fast acquisition scheme for achieving high-resolution MRS with J-scaling under inhomogeneous fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/2242293384859030748/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=2242293384859030748&amp;isPopup=true' title='2 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2242293384859030748'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2242293384859030748'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2009/03/fast-acquisition-scheme-for-achieving.html' title='Fast acquisition scheme for achieving high-resolution MRS with J-scaling under inhomogeneous fields'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>2</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-547074467258127633</id><published>2009-02-13T09:29:00.001-06:00</published><updated>2009-02-13T09:30:49.267-06:00</updated><title type='text'>iDQC anisotropy map imaging for tumor tissue characterization in vivo</title><content type='html'>Rosa T. Branca, Yuming M. Chen, Vladimir Mouraviev, Gigi Galiana, Elizabeth R. Jenista, Challa Kumar, Carola Leuschner, Warren S. Warren&lt;br /&gt;&lt;br /&gt;Intermolecular double quantum coherences (iDQCs), signals that result from simultaneous transitions of two or more separated spins, are known to produce images that are highly sensitive to subvoxel structure, particularly local anisotropy. Here we demonstrate how iDQCs signal can be used to efficiently detect the anisotropy created in breast tumor tissues and prostate tumor tissues by targeted (LHRH-conjugated) superparamagnetic nanoparticles (SPIONs), thereby distinguishing the necrotic area from the surrounding tumor tissue. Magn Reson Med, 2009. © 2009 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-547074467258127633?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21925' title='iDQC anisotropy map imaging for tumor tissue characterization in vivo'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/547074467258127633/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=547074467258127633&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/547074467258127633'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/547074467258127633'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2009/02/idqc-anisotropy-map-imaging-for-tumor.html' title='iDQC anisotropy map imaging for tumor tissue characterization in vivo'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-8751103894903501309</id><published>2008-10-21T10:41:00.000-05:00</published><updated>2008-10-21T10:42:39.481-05:00</updated><title type='text'>Hyperpolarized carbon–carbon intermolecular multiple quantum coherences</title><content type='html'>Journal of Magnetic Resonance&lt;br /&gt;Article in Press, Corrected Proof&lt;br /&gt;&lt;br /&gt;Hyperpolarized carbon–carbon intermolecular multiple quantum coherences&lt;br /&gt;&lt;br /&gt;Elizabeth R. JenistaCorresponding Author Contact Information, a, E-mail The Corresponding Author, Rosa T. Brancaa and Warren S. Warrena&lt;br /&gt;aCenter for Molecular and Biomolecular Imaging, 2220 French Family Science Center, Duke University, Durham, NC 27708, USA&lt;br /&gt;&lt;br /&gt;Received 17 July 2008; &lt;br /&gt;revised 17 September 2008. &lt;br /&gt;Available online 2 October 2008.&lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;&lt;br /&gt;Intermolecular multiple quantum coherences (iMQCs) can provide unique contrast with sub-voxel resolution. However, the characteristic growth rate of iMQCs mostly limits these effects to either hydrogen or hydrogen-coupled systems for thermally polarized samples. Hyperpolarization techniques such as dynamic nuclear polarization (DNP) allow for significant increases in the carbon signal (even more signal than that from hydrogen), making carbon iMQCs achievable. We present the first intermolecular multiple quantum signal between two carbon nuclei.&lt;br /&gt;&lt;br /&gt;Keywords: Intermolecular multiple quantum coherence; 13C hyperpolarization; Dynamic nuclear polarization; MultiCRAZED; CRAZED&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-8751103894903501309?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2008.09.027' title='Hyperpolarized carbon–carbon intermolecular multiple quantum coherences'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/8751103894903501309/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=8751103894903501309&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8751103894903501309'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8751103894903501309'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/10/hyperpolarized-carboncarbon.html' title='Hyperpolarized carbon–carbon intermolecular multiple quantum coherences'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4751622708882835917</id><published>2008-10-21T08:23:00.001-05:00</published><updated>2008-10-21T08:25:17.670-05:00</updated><title type='text'>Accurate Temperature Imaging Based on Intermolecular Coherences in Magnetic Resonance</title><content type='html'>Science 17 October 2008:&lt;br /&gt;Vol. 322. no. 5900, pp. 421 - 424&lt;br /&gt;DOI: 10.1126/science.1163242&lt;br /&gt; &lt;br /&gt;Accurate Temperature Imaging Based on Intermolecular Coherences in Magnetic Resonance&lt;br /&gt;Gigi Galiana, Rosa T. Branca, Elizabeth R. Jenista, and Warren S. Warren&lt;br /&gt;&lt;br /&gt;Conventional magnetic resonance methods that provide interior temperature profiles, which find use in clinical applications such as hyperthermic therapy, can develop inaccuracies caused by the inherently inhomogeneous magnetic field within tissues or by probe dynamics, and work poorly in important applications such as fatty tissues. We present a magnetic resonance method that is suitable for imaging temperature in a wide range of environments. It uses the inherently sharp resonances of intermolecular zero-quantum coherences, in this case flipping up a water spin while flipping down a nearby fat spin. We show that this method can rapidly and accurately assign temperatures in vivo on an absolute scale.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4751622708882835917?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1126/science.1163242' title='Accurate Temperature Imaging Based on Intermolecular Coherences in Magnetic Resonance'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4751622708882835917/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4751622708882835917&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4751622708882835917'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4751622708882835917'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/10/accurate-temperature-imaging-based-on.html' title='Accurate Temperature Imaging Based on Intermolecular Coherences in Magnetic Resonance'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4425444188911567253</id><published>2008-10-21T08:14:00.001-05:00</published><updated>2008-10-21T08:22:44.908-05:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Science Daily'/><title type='text'>Innovations Improve Accuracy Of MRI As Internal 'Thermometer'; Technique Can Enhance Cancer Therapy</title><content type='html'>ScienceDaily (Oct. 21, 2008) — Duke University chemists say they have developed a new way to measure temperature changes inside the body with unprecedented precision by correcting a subtle error in the original theory underlying Magnetic Resonance Imaging (MRI)...&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4425444188911567253?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www.sciencedaily.com/releases/2008/10/081016141455.htm' title='Innovations Improve Accuracy Of MRI As Internal &apos;Thermometer&apos;; Technique Can Enhance Cancer Therapy'/><link rel='enclosure' type='' href='http://dx.doi.org/10.1126/science.1163242' length='0'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4425444188911567253/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4425444188911567253&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4425444188911567253'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4425444188911567253'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/10/innovations-improve-accuracy-of-mri-as.html' title='Innovations Improve Accuracy Of MRI As Internal &apos;Thermometer&apos;; Technique Can Enhance Cancer Therapy'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1618017596847705102</id><published>2008-09-25T09:58:00.000-05:00</published><updated>2008-09-25T10:00:07.025-05:00</updated><title type='text'>BOLD imaging in the mouse brain using a turboCRAZED sequence at high magnetic fields</title><content type='html'>Johannes T. Schneider, Cornelius Faber&lt;br /&gt;&lt;br /&gt;Functional MRI (fMRI) based on the detection of intermolecular double-quantum coherences (iDQC) has previously been shown to provide pronounced activation signal. For fMRI in small animals at very high magnetic fields, the essential fast gradient echo-based readout methods become problematic. Here, rapid intermolecular double-quantum coherence (iDQC) imaging was implemented, combining the iDQC preparation sequence with a Turbo spin echo-like readout. Four-step phase cycling and a novel intensity-ordered k-space encoding scheme with separate acquisition of odd and even echoes were essential to optimize signal to noise ratio efficiency. Compared with a single echo readout of iDQC signal, acceleration of factor 16 was achieved in phantoms using the novel method at 17.6 Tesla. In vivo, echo trains consisting of 32 echoes were possible and images of the mouse brain were obtained in 30 s. The blood oxygen level dependent (BOLD) effect in the mouse brain upon change of breathing gas was observed as average signal change of (6.3 ± 1.1)% in iDQC images. Signal changes in conventional multi spin echo images were (4.4 ± 2.3)% and (8.3 ± 3.8)% with gradient echo methods. Combination of T2*-weighting with the fast iDQC sequence may yield higher signal changes than with either method alone, and establish fast iDQC imaging a robust tool for high field fMRI in small animals. Magn Reson Med 60:850-859, 2008. © 2008 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1618017596847705102?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21716' title='BOLD imaging in the mouse brain using a turboCRAZED sequence at high magnetic fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1618017596847705102/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1618017596847705102&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1618017596847705102'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1618017596847705102'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/09/bold-imaging-in-mouse-brain-using.html' title='BOLD imaging in the mouse brain using a turboCRAZED sequence at high magnetic fields'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1995524201763804199</id><published>2008-08-13T00:19:00.001-05:00</published><updated>2008-08-13T00:21:07.690-05:00</updated><title type='text'>Enhanced nonlinear magnetic resonance signals via square wave dipolar fields</title><content type='html'>R. T. Branca,1 G. Galiana,1,2 and W. S. Warren1&lt;br /&gt;1Center for Molecular and Biomolecular Imaging, Duke University, Durham, North Carolina 27708, USA&lt;br /&gt;2Chemistry Department, Princeton University, Princeton, New Jersey 08544, USA&lt;br /&gt;J. Chem. Phys. 129, 054502 (2008)&lt;br /&gt;&lt;br /&gt;This report introduces a new approach that enhances nonlinear solution magnetic resonance signals from intermolecular dipolar interactions. The resulting signals can theoretically be as large as the full equilibrium magnetization. Simple, readily implemented pulse sequences using square-wave magnetization modulation simultaneously refocus all even order intermolecular multiple quantum coherences, leading to a substantial net signal enhancement, complex nonlinear dynamics, and improved structural sensitivity under realistic conditions. ©2008 American Institute of Physics&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1995524201763804199?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1063/1.2962976' title='Enhanced nonlinear magnetic resonance signals via square wave dipolar fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1995524201763804199/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1995524201763804199&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1995524201763804199'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1995524201763804199'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/08/enhanced-nonlinear-magnetic-resonance.html' title='Enhanced nonlinear magnetic resonance signals via square wave dipolar fields'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1218164718547857296</id><published>2008-07-24T18:22:00.002-05:00</published><updated>2008-07-25T10:25:30.174-05:00</updated><title type='text'>Appendices A and B with mathematical derivations as referred to in the text (10 pages)</title><content type='html'>&lt;pre&gt;ARTICLE INFORMATION&lt;br /&gt;&lt;br /&gt;EPAPS Document No.: E-JCPSA6-129-617827&lt;br /&gt;&lt;br /&gt;Journal: J. Chem. Phys. 129, 044505 (2008)&lt;br /&gt;&lt;br /&gt;All Authors: Stefan Kirsch, William E. Hull&lt;br /&gt;&lt;br /&gt;Title: Quantitative time- and frequency-domain analysis of the two-pulse&lt;br /&gt;CRAZED NMR experiment; theoretical and experimental aspects, time-zero&lt;br /&gt;data truncation artefacts, and radiation damping&lt;br /&gt;&lt;br /&gt;Deposit Information&lt;br /&gt;&lt;br /&gt;Description: Appendices A and B with mathematical derivations as referred&lt;br /&gt;to in the text (10 pages)&lt;br /&gt;&lt;br /&gt;Total No. of Files: 2&lt;br /&gt;&lt;br /&gt;File Names: Readme.txt, 617827JCP appendices.pdf&lt;br /&gt;&lt;br /&gt;File Types: .txt and .pdf&lt;br /&gt;&lt;br /&gt;Contact:&lt;br /&gt;Dr. William E. Hull (PhD)&lt;br /&gt;Core Facility: Molecular Structure Analysis (W160)&lt;br /&gt;German Cancer Research Center (DKFZ)&lt;br /&gt;Im Neuenheimer Feld 280&lt;br /&gt;Postfach 101949&lt;br /&gt;D-69009 Heidelberg&lt;br /&gt;&lt;br /&gt;Fax: +49-6221-42-4554&lt;br /&gt;Tel: +49-6221-42-4515 / -4544 / -4542&lt;/pre&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1218164718547857296?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://ftp.aip.org/epaps/journ_chem_phys/E-JCPSA6-129-617827/' title='Appendices A and B with mathematical derivations as referred to in the text (10 pages)'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1218164718547857296/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1218164718547857296&amp;isPopup=true' title='2 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1218164718547857296'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1218164718547857296'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/07/appendices-and-b-with-mathematical.html' title='Appendices A and B with mathematical derivations as referred to in the text (10 pages)'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>2</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-5072001047310740244</id><published>2008-07-24T18:16:00.000-05:00</published><updated>2008-07-24T18:18:51.803-05:00</updated><title type='text'>Quantitative time- and frequency-domain analysis of the two-pulse COSY revamped by asymmetric Z-gradient echo detection NMR experiment: Theoretical an</title><content type='html'>&lt;h3&gt;&lt;a href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=JCPSA6&amp;amp;possible1=Kirsch%2C+Stefan&amp;amp;possible1zone=author&amp;amp;maxdisp=25&amp;amp;smode=strresults&amp;amp;aqs=true"&gt;&lt;/a&gt;&lt;/h3&gt;Stefan Kirsch and William E. Hull        &lt;br /&gt;J. Chem. Phys. 129, 044505 (2008)&lt;br /&gt;&lt;br /&gt;           The&lt;sup&gt; &lt;/sup&gt;two-pulse COSY revamped by asymmetric &lt;i&gt;Z&lt;/i&gt;-gradient echo detection (CRAZED) NMR&lt;sup&gt; &lt;/sup&gt;experiment has the basic form 90°−&lt;i&gt;G&lt;/i&gt;&lt;img src="http://scitation.aip.org/stockgif3/dgr.gif" alt="delta" align="bottom" border="0" /&gt;−&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;rec&lt;/sub&gt;−&lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;−&lt;i&gt;n&lt;/i&gt;&lt;i&gt;G&lt;/i&gt;&lt;img src="http://scitation.aip.org/stockgif3/dgr.gif" alt="delta" align="bottom" border="0" /&gt;−&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;rec&lt;/sub&gt;-FID, with a phase-encoding gradient&lt;sup&gt; &lt;/sup&gt;pulse &lt;i&gt;G&lt;/i&gt; of length &lt;img src="http://scitation.aip.org/stockgif3/dgr.gif" alt="delta" align="bottom" border="0" /&gt; applied during the evolution time&lt;sup&gt; &lt;/sup&gt;&lt;img src="http://scitation.aip.org/stockgif3/tgr.gif" alt="tau" align="bottom" border="0" /&gt; for transverse magnetization, readout pulse &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;, rephasing gradient &lt;i&gt;n&lt;/i&gt;&lt;i&gt;G&lt;/i&gt;&lt;img src="http://scitation.aip.org/stockgif3/dgr.gif" alt="delta" align="bottom" border="0" /&gt;,&lt;sup&gt; &lt;/sup&gt;and recovery time &lt;i&gt;t&lt;/i&gt;&lt;sub&gt;rec&lt;/sub&gt; prior to acquisition of the free-induction&lt;sup&gt; &lt;/sup&gt;decay. Based on the classical treatment of the spatially modulated&lt;sup&gt; &lt;/sup&gt;dipolar demagnetizing field and &lt;i&gt;without&lt;/i&gt; invoking intermolecular multiple-quantum coherence, a&lt;sup&gt; &lt;/sup&gt;new formulation of the first-order approximation for the theoretical solution&lt;sup&gt; &lt;/sup&gt;of the nonlinear Bloch equations has been developed. The &lt;i&gt;n&lt;/i&gt;th-order&lt;sup&gt; &lt;/sup&gt;CRAZED signal can be expressed as a simple product of&lt;sup&gt; &lt;/sup&gt;a scaling function &lt;i&gt;C&lt;/i&gt;&lt;sub&gt;&lt;i&gt;n&lt;/i&gt;&lt;/sub&gt;(&lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;,&lt;img src="http://scitation.aip.org/stockgif3/tgr.gif" alt="tau" align="bottom" border="0" /&gt;) and a signal amplitude function &lt;i&gt;A&lt;/i&gt;&lt;sub&gt;&lt;i&gt;n&lt;/i&gt;&lt;/sub&gt;(&lt;i&gt;t&lt;/i&gt;),&lt;sup&gt; &lt;/sup&gt;where the domain &lt;i&gt;t&lt;/i&gt; begins immediately after the &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt; pulse.&lt;sup&gt; &lt;/sup&gt;Using a &lt;i&gt;single-quantum&lt;/i&gt; coherence model, a generalized rf phase shift&lt;sup&gt; &lt;/sup&gt;function has also been developed, which explains all known phase&lt;sup&gt; &lt;/sup&gt;behavior, including &lt;i&gt;n&lt;/i&gt;th-order echo selection by phase cycling. Details of&lt;sup&gt; &lt;/sup&gt;the derivations are provided in two appendices as supplementary material.&lt;sup&gt; &lt;/sup&gt;For &lt;i&gt;n&lt;/i&gt;&gt;1, &lt;i&gt;A&lt;/i&gt;&lt;sub&gt;&lt;i&gt;n&lt;/i&gt;&lt;/sub&gt;(&lt;i&gt;t&lt;/i&gt;) increases from zero to a maximum value&lt;sup&gt; &lt;/sup&gt;at &lt;i&gt;t&lt;/i&gt;=&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;max&lt;/sub&gt; before decaying and can be expressed as a&lt;sup&gt; &lt;/sup&gt;series of &lt;i&gt;n&lt;/i&gt; exponential decays with antisymmetric binomial coefficients. Fourier&lt;sup&gt; &lt;/sup&gt;transform gives an antisymmetric binomial series of Lorentzians, where the&lt;sup&gt; &lt;/sup&gt;composite lineshape exhibits negative wings, zero integral, and a linewidth&lt;sup&gt; &lt;/sup&gt;that decreases with &lt;i&gt;n&lt;/i&gt;. Analytical functions are presented for &lt;i&gt;t&lt;/i&gt;&lt;sub&gt;max&lt;/sub&gt;&lt;sup&gt; &lt;/sup&gt;and &lt;i&gt;A&lt;/i&gt;&lt;sub&gt;&lt;i&gt;n&lt;/i&gt;&lt;/sub&gt;(&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;max&lt;/sub&gt;) and for estimating the maximal percent error incurred&lt;sup&gt; &lt;/sup&gt;for &lt;i&gt;A&lt;/i&gt;&lt;sub&gt;&lt;i&gt;n&lt;/i&gt;&lt;/sub&gt;(&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;max&lt;/sub&gt;) when using the first-order model. The preacquisition delay&lt;sup&gt; &lt;/sup&gt;&lt;img src="http://scitation.aip.org/stockgif3/Dgr.gif" alt="Delta" align="bottom" border="0" /&gt;=&lt;img src="http://scitation.aip.org/stockgif3/dgr.gif" alt="delta" align="bottom" border="0" /&gt;+&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;rec&lt;/sub&gt; results in the loss of the data points for&lt;sup&gt; &lt;/sup&gt;&lt;i&gt;t&lt;/i&gt;=0 to &lt;img src="http://scitation.aip.org/stockgif3/Dgr.gif" alt="Delta" align="bottom" border="0" /&gt;. Conventional Fourier transformation produces time-zero truncation artifacts&lt;sup&gt; &lt;/sup&gt;(reduced negative wing amplitude, nonzero integral, and reduced effective &lt;i&gt;T&lt;/i&gt;&lt;img src="http://scitation.aip.org/servlet/GetImg?key=JCPSA6000129000004044505000001%3A0%3A0%3A28&amp;amp;t=a&amp;amp;d=a" alt="" /&gt;2&lt;/sub&gt;&lt;sup&gt; *&lt;/sup&gt;" align="middle" border="0"&gt;),&lt;sup&gt; &lt;/sup&gt;which can be avoided by time-domain fitting after right shifting&lt;sup&gt; &lt;/sup&gt;the data by &lt;img src="http://scitation.aip.org/stockgif3/Dgr.gif" alt="Delta" align="bottom" border="0" /&gt;. A doped water sample (9.93 mM&lt;sup&gt; &lt;/sup&gt;NiSO&lt;sub&gt;4&lt;/sub&gt;, 10 mm sample tube) was used to study the&lt;sup&gt; &lt;/sup&gt;behavior of the CRAZED signal for &lt;i&gt;n&lt;/i&gt;=1–4 with &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;=90° at&lt;sup&gt; &lt;/sup&gt;7 T (300 MHz &lt;sup&gt;1&lt;/sup&gt;H frequency) as a function of&lt;sup&gt; &lt;/sup&gt;&lt;img src="http://scitation.aip.org/stockgif3/Dgr.gif" alt="Delta" align="bottom" border="0" /&gt;, with and without radiation damping. Pulse-acquire experiments were used&lt;sup&gt; &lt;/sup&gt;to determine the relaxation times (&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;=61.8  ms and &lt;i&gt;T&lt;/i&gt;&lt;img src="http://scitation.aip.org/servlet/GetImg?key=JCPSA6000129000004044505000001%3A0%3A0%3A28&amp;amp;t=a&amp;amp;d=a" alt="" /&gt;2&lt;/sub&gt;&lt;sup&gt; *&lt;/sup&gt;" align="middle" border="0"&gt;=29.7  ms), and the&lt;sup&gt; &lt;/sup&gt;radiation damping time constant &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;rd&lt;/sub&gt;=18.5  ms. When experimental CRAZED data sets&lt;sup&gt; &lt;/sup&gt;were right shifted by &lt;img src="http://scitation.aip.org/stockgif3/Dgr.gif" alt="Delta" align="bottom" border="0" /&gt;, excellent least-squares fits to the&lt;sup&gt; &lt;/sup&gt;first-order model function were obtained for all &lt;i&gt;n&lt;/i&gt; using a&lt;sup&gt; &lt;/sup&gt;minimal set of free variables. Without radiation damping the fitted&lt;sup&gt; &lt;/sup&gt;&lt;i&gt;T&lt;/i&gt;&lt;img src="http://scitation.aip.org/servlet/GetImg?key=JCPSA6000129000004044505000001%3A0%3A0%3A28&amp;amp;t=a&amp;amp;d=a" alt="" /&gt;2&lt;/sub&gt;&lt;sup&gt; *&lt;/sup&gt;" align="middle" border="0"&gt;values (29.7–30.2 ms) agreed with the reference value. With radiation&lt;sup&gt; &lt;/sup&gt;damping the fitted effective &lt;i&gt;T&lt;/i&gt;&lt;img src="http://scitation.aip.org/servlet/GetImg?key=JCPSA6000129000004044505000001%3A0%3A0%3A28&amp;amp;t=a&amp;amp;d=a" alt="" /&gt;2&lt;/sub&gt;&lt;sup&gt; *&lt;/sup&gt;" align="middle" border="0"&gt; values were 16.2 ms for&lt;sup&gt; &lt;/sup&gt;a 90° pulse-acquire experiment and 18.8–20.2 ms for the CRAZED&lt;sup&gt; &lt;/sup&gt;experiment with &lt;i&gt;n&lt;/i&gt;=1–4 and signal amplitudes spanning a range of&lt;sup&gt; &lt;/sup&gt;10&lt;sup&gt;5&lt;/sup&gt;. ©2008 &lt;i&gt;American Institute of Physics&lt;/i&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;h3&gt;&lt;/h3&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-5072001047310740244?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1063/1.2951993' title='Quantitative time- and frequency-domain analysis of the two-pulse COSY revamped by asymmetric Z-gradient echo detection NMR experiment: Theoretical an'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/5072001047310740244/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=5072001047310740244&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5072001047310740244'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5072001047310740244'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/07/quantitative-time-and-frequency-domain.html' title='Quantitative time- and frequency-domain analysis of the two-pulse COSY revamped by asymmetric Z-gradient echo detection NMR experiment: Theoretical an'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-988521932259433197</id><published>2008-05-19T11:52:00.002-05:00</published><updated>2008-05-19T11:55:32.044-05:00</updated><title type='text'>Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)</title><content type='html'>Stefan Kirsch and Peter Bachert&lt;br /&gt;Journal of Magnetic Resonance&lt;br /&gt;   Volume 185, Issue 2,    April 2007,   Pages 183-190&lt;br /&gt;&lt;br /&gt;In the CRAZED experiment (COSY revamped by asymmetric Z-gradient echo detection, Warren et al.), a spatially anisotropic magnetization distribution is created by application of a magnetic field gradient (strength G, duration τ) which in turn generates a response called the distant dipolar field (DDF). The DDF is a source of intermolecular multiple-quantum coherences (iMQC) which contain information on the distance d = π/(γGτ) between pairs of dipolar-coupled spins. Diffraction-like phenomena may result for periodically structured samples. In this study, we report the observation of diffraction owing to the DDF at 1.5 T using a clinical whole-body tomograph. Based on the semi-classical treatment of the problem by Robyr and Bowtell, diffraction conditions were obtained for a CRAZED-type pulse sequence that selects iMQC of order N. The predicted distinct difference in N = 2 and N ≠ 2 coherences, i.e., a dominant continuous course as a function of τ (N = 2) and prominent diffraction peaks otherwise, could be verified in CRAZED experiments in a periodically structured sample selecting coherence orders N = 2 and N = 3. The diffractive signal component contains information on the geometric structure of the sample. Applications of this technique may permit the detection of changes in composition and geometry of periodic structures.    Keywords: CRAZED; Distant dipolar field (DDF); Intermolecular multiple-quantum coherence; Diffraction&lt;div style="display: inline;" class="articleText"&gt;&lt;p&gt;&lt;/p&gt; &lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-988521932259433197?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2006.10.011' title='Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/988521932259433197/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=988521932259433197&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/988521932259433197'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/988521932259433197'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/diffraction-like-phenomena-in-periodic.html' title='Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-5960577943331556918</id><published>2008-05-15T10:32:00.002-05:00</published><updated>2008-05-15T10:35:36.366-05:00</updated><title type='text'>Localized intermolecular zero-quantum coherence spectroscopy in vivo</title><content type='html'>David Z. Balla , Cornelius Faber&lt;br /&gt;Concepts in Magnetic Resonance Part A&lt;br /&gt;Volume 32A, Issue 2 , Pages 117 - 133&lt;br /&gt;&lt;br /&gt;Resolution enhancement in NMR spectra, acquired in spatially or temporally varying magnetic fields, can be achieved with 2D pulse sequences detecting intermolecular zero-quantum coherences (iZQC). The insensitivity towards long range field distortions renders these methods particularly appealing for in vivo NMR spectroscopy, where ample sources of field inhomogeneities are encountered. This article provides a comprehensive description of iZQC spectroscopy, following a classical treatment. A pictorial explanation is given of how iZQC signal is formed under the action of the distant dipolar field in the sample and how this local refocusing process leads to line narrowing in the indirect dimension of 2D spectra. Signal evolution and peak positions in the spectra are analyzed by solving the modified Bloch equations. Finally, it is explained how water suppression and localization can be combined with the iZQC preparation sequence, and recent in vivo applications are discussed. The given examples illustrate that iZQC spectroscopy can provide either resolution or sensitivity enhancement in vivo. © 2008 Wiley Periodicals, Inc. Concepts Magn Reson Part A 32A: 117-133, 2008.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-5960577943331556918?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/cmr.a.20104' title='Localized intermolecular zero-quantum coherence spectroscopy in vivo'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/5960577943331556918/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=5960577943331556918&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5960577943331556918'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5960577943331556918'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/localized-intermolecular-zero-quantum.html' title='Localized intermolecular zero-quantum coherence spectroscopy in vivo'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-8761943569002455811</id><published>2008-05-13T10:04:00.002-05:00</published><updated>2008-05-13T10:25:22.268-05:00</updated><title type='text'>Intermolecular zero-quantum coherence NMR spectroscopy in the presence of local dipole fields
spectroscopy in vivo</title><content type='html'>&lt;a href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=ALL&amp;amp;possible1=Balla%2C+David+Z.&amp;amp;possible1zone=author&amp;amp;maxdisp=25&amp;amp;smode=strresults&amp;amp;aqs=true"&gt;&lt;/a&gt;David Z. Balla and Cornelius Faber&lt;br /&gt;Department of Experimental Physics 5, University of Würzburg, 97074 Würzburg, Germany&lt;br /&gt;       J. Chem. Phys. 128, 154522 (2008);    DOI:10.1063/1.2904564&lt;h3&gt;&lt;/h3&gt;NMR&lt;sup&gt; &lt;/sup&gt;experiments detecting intermolecular zero-quantum coherences (iZQCs) allow for observation of&lt;sup&gt; &lt;/sup&gt;homogeneous line shapes under inhomogeneous magnetic fields. Local dipole fields&lt;sup&gt; &lt;/sup&gt;impair the refocusing capacity of such experiments and render the&lt;sup&gt; &lt;/sup&gt;available theoretical description of signal evolution invalid. In this article,&lt;sup&gt; &lt;/sup&gt;the impact of local dipole fields on two-dimensional iZQC spectroscopy&lt;sup&gt; &lt;/sup&gt;experiments was assessed by performing extensive numerical simulations, which solved&lt;sup&gt; &lt;/sup&gt;the nonlinear Bloch equations for a binary solution in a&lt;sup&gt; &lt;/sup&gt;magnetization array of 64&lt;sup&gt;3&lt;/sup&gt; spatial points. Local dipole fields were&lt;sup&gt; &lt;/sup&gt;simulated using spherical volumes with different magnetic susceptibility values corresponding&lt;sup&gt; &lt;/sup&gt;to either a glass sphere or an air inclusion with&lt;sup&gt; &lt;/sup&gt;a diameter of 100  &lt;i&gt;µ&lt;/i&gt;m. The local field resulted in a&lt;sup&gt; &lt;/sup&gt;broadened distribution of difference frequencies between locally interacting spins and&lt;sup&gt; &lt;/sup&gt;led to the dominating effect of decreasing the amplitude of&lt;sup&gt; &lt;/sup&gt;the solute peak, before line broadening was observed in the&lt;sup&gt; &lt;/sup&gt;spectra. From simulations using a magnetic field strength of 17.6  T,&lt;sup&gt; &lt;/sup&gt;the smallest ratio of sample to inclusion volume that still&lt;sup&gt; &lt;/sup&gt;allowed for observation of the solute peak was determined to&lt;sup&gt; &lt;/sup&gt;be &lt;img src="http://scitation.aip.org/stockgif3/eegr.gif" alt="eta" align="middle" border="0" /&gt;&lt;sub&gt;limit&lt;/sub&gt;=215 and &lt;img src="http://scitation.aip.org/stockgif3/eegr.gif" alt="eta" align="middle" border="0" /&gt;&lt;sub&gt;limit&lt;/sub&gt;=392 for glass and air inclusions, respectively.&lt;sup&gt; &lt;/sup&gt;Experimental data acquired with a 100  &lt;i&gt;µ&lt;/i&gt;m diameter glass sphere embedded&lt;sup&gt; &lt;/sup&gt;in agar gel yielded a value of &lt;img src="http://scitation.aip.org/stockgif3/eegr.gif" alt="eta" align="middle" border="0" /&gt;&lt;sub&gt;limit&lt;/sub&gt;=252 and confirmed&lt;sup&gt; &lt;/sup&gt;the order of magnitude obtained from the simulations. From these&lt;sup&gt; &lt;/sup&gt;data, it was concluded that iZQC spectroscopy is possible as&lt;sup&gt; &lt;/sup&gt;long as the relative volume occupied by air inclusions does&lt;sup&gt; &lt;/sup&gt;not exceed the order of 0.1% of the sample volume.&lt;sup&gt; &lt;/sup&gt;This limit, in contrast to the previous speculations, strongly excludes&lt;sup&gt; &lt;/sup&gt;materials or tissues with high density of strong inhomogeneities from&lt;sup&gt; &lt;/sup&gt;the investigation by iZQC spectroscopy. ©2008 &lt;i&gt;American Institute of Physics&lt;/i&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-8761943569002455811?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1063/1.2904564' title='Intermolecular zero-quantum coherence NMR spectroscopy in the presence of local dipole fields&#xA;spectroscopy in vivo'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/8761943569002455811/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=8761943569002455811&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8761943569002455811'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8761943569002455811'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/intermolecular-zero-quantum-coherence.html' title='Intermolecular zero-quantum coherence NMR spectroscopy in the presence of local dipole fields&#xA;spectroscopy in vivo'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-2810111701251700637</id><published>2008-05-13T10:02:00.001-05:00</published><updated>2008-05-13T10:04:00.623-05:00</updated><title type='text'>In vivo intermolecular zero-quantum coherence MR spectroscopy in the rat spinal cord at 17.6 T: a feasibility study</title><content type='html'>&lt;p class="AuthorGroup"&gt;David Z. Balla&lt;sup&gt;1, 2&lt;/sup&gt; and Cornelius Faber&lt;sup&gt;1 &lt;a href="http://www.springerlink.com/content/v8362054721244g0/#ContactOfAuthor2"&gt;&lt;img alt="Contact Information" src="http://www.springerlink.com/images/contact.gif" border="0" /&gt;&lt;/a&gt;&lt;/sup&gt;&lt;/p&gt;       &lt;table&gt;          &lt;tbody&gt;             &lt;tr valign="top"&gt;                &lt;td&gt;&lt;span class="Affiliation"&gt;&lt;a name="Aff1"&gt;&lt;/a&gt;(1) &lt;/span&gt;&lt;/td&gt;                &lt;td&gt;&lt;span class="Affiliation"&gt;Department of Experimental Physics 5, University of Würzburg, Am Hubland, 97074 Würzburg, Germany&lt;/span&gt;&lt;/td&gt;             &lt;/tr&gt;          &lt;/tbody&gt;       &lt;/table&gt;       &lt;table&gt;          &lt;tbody&gt;             &lt;tr valign="top"&gt;                &lt;td&gt;&lt;span class="Affiliation"&gt;&lt;a name="Aff2"&gt;&lt;/a&gt;(2) &lt;/span&gt;&lt;/td&gt;                &lt;td&gt;&lt;span class="Affiliation"&gt;&lt;i&gt;Present address: &lt;/i&gt;Max-Planck-Institute for Biological Cybernetics, 72076 Tübingen, Germany&lt;/span&gt;&lt;/td&gt;             &lt;/tr&gt;          &lt;/tbody&gt;       &lt;/table&gt;       &lt;p class="Affiliation"&gt;&lt;strong&gt;Received: &lt;/strong&gt;5 April 2007  &lt;strong&gt;Revised: &lt;/strong&gt;14 August 2007  &lt;strong&gt;Accepted: &lt;/strong&gt;17 August 2007  &lt;strong&gt;Published online: &lt;/strong&gt;18 September 2007       &lt;/p&gt;       &lt;div class="Abstract"&gt;&lt;a name="Abs1"&gt;&lt;/a&gt;&lt;span class="AbstractHeading"&gt;Abstract&lt;/span&gt;&lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec1"&gt;&lt;/a&gt;Objective:  &lt;/span&gt;The feasibility of in vivo magnetic resonance spectroscopy of the healthy rat spinal cord at 17.6 T using conventional methods and intermolecular zero-quantum coherence (iZQC) spectroscopy is explored and the performance of both approaches is compared. &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec2"&gt;&lt;/a&gt;Methods:  &lt;/span&gt;Localised spectra were acquired at 17.6 T from three healthy Fisher rats and phantoms with injected iron-oxide particles using                the PRESS and a modified HOMOGENIZED sequence.             &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec3"&gt;&lt;/a&gt;Results:  &lt;/span&gt;Well-resolved in vivo spectra showing the four singlet resonances of creatine, choline, and &lt;i&gt;N&lt;/i&gt;-acetyl aspartate were obtained with both approaches. iZQC spectra were acquired from larger voxels, but did not provide higher sensitivity or resolution in the healthy spinal cord. In the presence of paramagnetic iron-oxide particles, the quality of in vitro spectra acquired with PRESS declined and was strongly dependent on the quality of the local shim. iZQC spectra were not affected by the presence of iron-oxide particles and provided narrow lines (9 Hz) independent of the shim. &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec4"&gt;&lt;/a&gt;Conclusion:  &lt;/span&gt;In vivo iZQC spectroscopy of the rat spinal cord is possible. The robustness in presence of local field distortions makes iZQC methods a promising alternative for the investigation of tissue containing labelled cells, implants, or clotted blood. New application of MRS to tissue inaccessible using conventional methods may thus become possible. &lt;/div&gt;          &lt;/div&gt;       &lt;/div&gt;       &lt;p class="Keyword"&gt;&lt;span class="KeywordHeading"&gt;Keywords  &lt;/span&gt;MR spectroscopy - Resolution enhancement - iMQC - DDF - SPIO       &lt;/p&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-2810111701251700637?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1007/s10334-007-0081-3' title='In vivo intermolecular zero-quantum coherence MR spectroscopy in the rat spinal cord at 17.6 T: a feasibility study'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/2810111701251700637/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=2810111701251700637&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2810111701251700637'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2810111701251700637'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/in-vivo-intermolecular-zero-quantum.html' title='In vivo intermolecular zero-quantum coherence MR spectroscopy in the rat spinal cord at 17.6 T: a feasibility study'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4346444816166813084</id><published>2008-05-11T00:02:00.002-05:00</published><updated>2008-05-11T00:06:54.530-05:00</updated><title type='text'>Understanding intra- and intermolecular multiple quantum coherences</title><content type='html'>This was in the weekend educational program.&lt;br /&gt;Somebody registered for the weekend must login...&lt;br /&gt;&lt;br /&gt;_____________________________________&lt;br /&gt;&lt;br /&gt;MR Physics for Physicists&lt;br /&gt;Organizer: Michael H. Buonocore, M.D., Ph.D.&lt;br /&gt;Skill Level: Intermediate – Advanced&lt;br /&gt;Saturday, 3 May, 08:30 – 18:15, Room 801 A/B&lt;br /&gt;&lt;br /&gt;Spin Physics&lt;br /&gt;09:30 Understanding intra- and intermolecular multiple quantum coherences&lt;br /&gt;Jianhui Zhong, Ph.D.&lt;br /&gt;University of Rochester, USA&lt;br /&gt;&lt;br /&gt;Nuclear magnetic resonance (NMR), after all, is a quantum mechanical phenomenon.&lt;br /&gt;Even though in the imaging community, we are mostly familiar and use in most times the&lt;br /&gt;so-called vector model which describes the MR signal as from a precessing bar magnet&lt;br /&gt;inside the magnetic field (not too much different from a spinning toy top in the earth’s&lt;br /&gt;gravitation field), at a more fundamental level quantum mechanics should be used for&lt;br /&gt;NMR. The phenomena of multiple-quantum coherence (MQC) not only provides a nice&lt;br /&gt;demonstration of the true quantum mechanical nature of NMR, applications of various&lt;br /&gt;MQC techniques also reveal many interesting structural and functional information in&lt;br /&gt;MRS and MRI...&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4346444816166813084?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://cds.ismrm.org/syllabus-2008' title='Understanding intra- and intermolecular multiple quantum coherences'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4346444816166813084/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4346444816166813084&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4346444816166813084'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4346444816166813084'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/understanding-intra-and-intermolecular.html' title='Understanding intra- and intermolecular multiple quantum coherences'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-957732819445059622</id><published>2008-05-10T22:53:00.010-05:00</published><updated>2008-05-10T23:57:24.434-05:00</updated><title type='text'>ISMRM 2008 DDF/iMQC</title><content type='html'>Here are the iMQC/DDF related abstracts that I found. Please email me if I missed one (especially yours!) corum@cmrr.umn.edu&lt;br /&gt;&lt;br /&gt;Hopefully you, or a colleague has access to the login.&lt;br /&gt;&lt;br /&gt;Curt&lt;br /&gt;&lt;br /&gt;______________________________________&lt;br /&gt;&lt;br /&gt;1407.&lt;br /&gt;Intermolecular Zero-Quantum Coherence Imaging in Structured Samples&lt;br /&gt;Bernard Siow1, Li Sun1, Andrew M. Blamire1&lt;br /&gt;1Newcastle University, Newcastle upon Tyne, UK&lt;br /&gt;&lt;br /&gt;Intermolecular multiple quantum coherence imaging sequences have recently been shown to provide a fundamentally different contrast mechanism to conventional MRI. A numerical study of intermolecular zero-quantum coherence imaging has shown sensitivity to susceptibility gradients at selected distance scales. In this study, an iZQC sequence was implemented and iZQC signal verified. The sequence was used to investigate sensitivity to susceptibility gradients at selected distance scales in structured samples. Images show contrast in areas where susceptibility gradients are present. Furthermore, contrast was modulated by the distance scale selected. Further results suggest that contrast is modulated by specific resonant frequency difference at distance scale selected.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;div style="text-align: left;"&gt;1454.&lt;br /&gt;Fast Relaxation Induced by SPIO Compromises Contrast from Intermolecular Double–quantum Coherence in CRAZED–MRI&lt;br /&gt;Elvira Mehlin1, Stefan Kirsch1, Peter Bachert1&lt;br /&gt;1German Cancer Research Center (DKFZ), 69120 Heidelberg, Germany&lt;br /&gt;&lt;br /&gt;The CRAZED sequence permits detection of signal generated by intermolecular double–quantum coherence (iDQC). When applied to 1H MRI, a novel type of contrast is obtained, in particular, a positive contrast when superparamagnetic iron oxide particles (SPIOs) are present. We demonstrate that the high T1–relaxivity of SPIOs can cause spurious signal in CRAZED MRI which cannot be attributed to iDQC.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;1458.&lt;br /&gt;Optimization of Parameters for the Distant Dipolar Field Signal Acquired in CRAZED-Multiecho Pulse Sequence&lt;br /&gt;Chung Ki K. Wong1, Jianhui Zhong1&lt;br /&gt;1University of Rochester, Rochester, New York, USA&lt;br /&gt;&lt;br /&gt;The decrease of dipolar signal with refocusing pulses of finite duration in a CRAZED-multiecho acquisition was investigated previously. It was found that the rephasing of the dipolar signal during the refocusing pulses in the multiecho sequence depends substantially on the phase of the pulses. In this abstract, the total signal acquired from the multiecho sequence was optimized with the parameters of the sequence. The results show that the attenuation of the signal due to the finite duration of the refocusing pulses can be compensated with a longer τ2 and a proper  choice of the phase of the pulses.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;1562.&lt;br /&gt;Time-Zero Signal Truncation in CRAZED Experiments Due to Rephasing Gradient Delays Leads to Incorrect Frequency-Domain Lineshapes&lt;br /&gt;Stefan Kirsch1, William Edmund Hull1&lt;br /&gt;1German Cancer Research Center (DKFZ), Heidelberg, Germany&lt;br /&gt;&lt;br /&gt;In contrast to the decay of a conventional pulse-acquire FID, the time-domain signal from of a CRAZED-type pulse sequence for coherence order n &gt; 1 increases from initially zero to a maximum, followed by an exponential decay. We show that the finite duration of the coherence rephasing gradient and any subsequent recovery delays lead to loss of the initial portion of the time-domain signal. This so-called “time-zero truncation artefact” results in an altered frequency-domain lineshape with incorrect integral and linewidth. Correct analysis requires time-domain fitting of right-shifted data.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;1563.&lt;br /&gt;In Vivo Human Whole Cerebellum MRS Under Severe Field Inhomogeneity with IDQC Method&lt;br /&gt;Tianliang Gu1, 2, Zhong Chen1, Xiaoxu Liu1, Ling-chih Lin1, Jianhui Zhong1&lt;br /&gt;1University of Rochester, Rochester, New York, USA&lt;br /&gt;&lt;br /&gt;An intermolecular double quantum coherence (iDQC) 2D MRS pulse sequence was created and implemented on a 3T scanner for acquisition of human brain 1H spectra in regions susceptible to field inhomogeneity such as the cerebellum. High resolution 1D MRS could be obtained in a few minutes with iDQC over the whole cerebellum, whereas conventional single voxel 1D MRS was working successfully only when regions much smaller were covered. NAA/Cr and Cho/Cr measured with both methods in 5 healthy subjects agreed well with each other.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;2361.&lt;br /&gt;Enhanced BOLD Effect in the Mouse Brain with Fast CRAZED Imaging at High Magnetic Fields&lt;br /&gt;Johannes Thomas Schneider, Cornelius Faber&lt;br /&gt;&lt;br /&gt;A fast CRAZED sequence detecting the signal from intermolecular multiple-quantum coherences (iMQC) was implemented at 17.6 T to observe the BOLD effect in the mouse brain. Signal readout as echo train employing a four-step phase cycle for the refocusing pulses and an intensity-ordered k-space sampling allowed for acquisition of CRAZED images in 30 seconds. In the CRAZED images the BOLD effect was more pronounced than in RARE images but smaller than in gradient echo images. Combination of iMQC with T2*-effects may provide larger signal changes than conventional BOLD methods.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3063.&lt;br /&gt;Enhanced Contrast in CEST MRI Via Intermolecular Double Quantum Coherences&lt;br /&gt;Shengchun Zhang1, Huijun Sun1, Zhong Chen1, Congbo Cai1, Jianhui Zhong2&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China; 2University of Rochester, Rochester, New York, USA&lt;br /&gt;&lt;br /&gt;A CEST imaging technique based on intermolecular double quantum coherence (iDQC) is proposed. Quantitative analysis and experiments in glucose agarose-gel phantoms demonstrate that, in CEST MRI, iDQC signal is more sensitive to RF saturation than the conventional SQC signal, and thus needs RF saturation pulses of lower power to achieve similar CEST image contrast. Consequently, the method can reduce the potential RF burning in clinic applications, and is expected to facilitate the study of the CEST effect in the system with exchangeable protons of low concentrations.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3125.&lt;br /&gt;High-Resolution MR Spectroscopy in Inhomogeneous and Unstable Fields Via Intermolecular Zero-Quantum Coherences&lt;br /&gt;Xi Chen1, Meijin Lin1, Tao Lin1, Zhong Chen1, Jianhui Zhong2&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China; 2University of Rochester, Xiamen, New York, USA&lt;br /&gt;&lt;br /&gt;A new iZQC pulse sequence with stroboscopic acquisition is designed to achieve high-resolution magnetic resonance spectroscopy in inhomogeneous and unstable fields. Primary results suggest potential applications for suppressions of motion-caused t1 noises and inhomogeneous broadenings in in vivo studies.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3186.&lt;br /&gt;High Resolution NMR Spectra in Inhomogeneous Fields Via Intermolecular Multiple Quantum Coherences Without Coherence Selection Gradients&lt;br /&gt;Zhong Chen1, Congbo Cai1, Yanqin Lin1, Shuhui Cai1, Jianhui Zhong2&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China; 2University of Rochester, Rochester, New York, USA&lt;br /&gt;&lt;br /&gt;Coherence selection gradient has been thought to be essential for high resolution NMR spectra in inhomogeneous field based on intermolecular multiple quantum coherences (iMQC). However, our experimental results show that it can be omitted if correct phase cycling is applied. This means that the measured line-width of high resolution spectral peaks is not determined by the dipolar correlation distance caused by coherence selection gradient, but only affected by the effects of diffusion and T2 relaxation. This result prompts us to reconsider the iMQC high resolution mechanism.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3188.&lt;br /&gt;An Effective Fast Acquisition Scheme to Achieve High-Resolution MRS with J-Coupling Scaling Via Intermolecular Multiple-Quantum Coherences&lt;br /&gt;Xi Chen1, Meijin Lin1, Jincan Chen1, Tao Lin1, Zhong Chen1&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China&lt;br /&gt;&lt;br /&gt;A series of intermolecular double-quantum filtered (iDQF) sequence with efficient solvent suppression and different scaling factors of J-coupling constants, named iDQF-HOMOGENIZED II (abbreviated as iDH2), are designed to achieve fast acquisition of high-resolution spectra in inhomogeneous fields. Experiments on swine brain tissues were performed to test the feasibility of the new method. The results suggest potential applications for in vivo spectroscopy.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3189.&lt;br /&gt;A Flexible IMQC Method for Accurate Determination of J-Coupling Constants in  Inhomogeneous Fields&lt;br /&gt;Yanqin Lin1, Shuhui Cai1, Yuqing Huang1, Zhong Chen1, Jianhui Zhong2&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China; 2University of Rochester, Rochester, New York, USA&lt;br /&gt;&lt;br /&gt;An improved pulse sequence was developed to scale apparent J coupling constants by a scaling factor ranging theoretically from zero (completely decoupled) to infinity under inhomogeneous fields via intermolecular multiple-quantum coherences. Scaling up the apparent J coupling constants allows more accurate measurement of small J coupling constants, and a completely decoupled homonuclear spectrum can be of considerable help for improving signal separation and thus peak assignment in MRS. The resulting spectrum retains conventional high-resolution NMR spectral information.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3351.&lt;br /&gt;Apparent Diffusion Behaviors Modulated by Distant Dipolar Field in Solution NMR&lt;br /&gt;Shuhui Cai1, Guiping Shen1, Congbo Cai1, Zhong Chen1&lt;br /&gt;1Xiamen University, Xiamen, People's Republic of China&lt;br /&gt;&lt;br /&gt;A modified CRAZED sequence was designed to observe and characterize apparent diffusion behaviors of signals from intermolecular double-quantum coherences during the mixing period. It is found that their apparent diffusion behaviors are different from conventional single-quantum coherences, and different orientation of diffusion weighting gradients relative to coherence selection gradients results in different apparent diffusion behaviors. This indicates&lt;br /&gt;that the apparent diffusion behavior is influenced by the distant dipolar field.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;3647.&lt;br /&gt;Enhancement of MT, CEST and NOE Contrast Via Intermolecular Multiple Quantum Coherences&lt;br /&gt;Wen Ling1, Uzi Eliav1, Xu Yang2, Gil Navon1, Alexej Jerschow2&lt;br /&gt;1Tel Aviv University, Israel; 2New York University, New York, New York, USA&lt;br /&gt;&lt;br /&gt;We demonstrate that using intermolecular multiple-quantum coherences can enhance contrast in MTC/CEST/NOE experiments in proportion to (Mz/Mo)p, where Mz is the the saturated level of the z-component of the magnetization, Mo its value in equilibrium and l is the coherence order used. These methods are demonstrated on a series of glycosaminoglycan (GAG) samples, and also for a piece of bovine articular cartilage.&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-957732819445059622?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://submissions.miracd.net/ISMRM2008Proceedings/' title='ISMRM 2008 DDF/iMQC'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/957732819445059622/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=957732819445059622&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/957732819445059622'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/957732819445059622'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/ismrm-2008-ddfimqc.html' title='ISMRM 2008 DDF/iMQC'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-184220362530548405</id><published>2008-05-10T22:43:00.002-05:00</published><updated>2008-05-10T22:46:26.175-05:00</updated><title type='text'>High-resolution NMR spectra in inhomogeneous fields utilizing the CRAZED sequence without coherence selection gradients</title><content type='html'>&lt;div class="articleTitle"&gt;&lt;p&gt;&lt;/p&gt;&lt;/div&gt;Congbo Cai, Yanqin Lin, Shuhui Cai, Zhong Chen, ,  and Jianhui Zhong&lt;br /&gt;&lt;br /&gt;&lt;a href="http://www.sciencedirect.com.floyd.lib.umn.edu/science/journal/10907807"&gt;&lt;b&gt;&lt;/b&gt;&lt;/a&gt;Journal of Magnetic Resonance&lt;br /&gt;Article in Press, Corrected Proof&lt;br /&gt;&lt;br /&gt;Abstract: Coherence selection gradients have been considered as indispensable for high-resolution NMR spectroscopy in inhomogeneous fields utilizing the CRAZED-type sequences. However, our experimental results demonstrate that these gradients can be omitted if an appropriate phase cycling is applied. The measured linewidth of reconstructing 1D high-resolution spectral peaks does not depend on the dipolar correlation distance determined by the coherence selection gradients, but is only affected by diffusion and T2 relaxation. This finding suggests the need to reconsider the mechanism for the iMQC-based high-resolution spectroscopy.&lt;br /&gt;&lt;br /&gt;Keywords: High-resolution spectra; Intermolecular multiple-quantum coherences; Inhomogeneous fields; Dipolar correlation distance; Coherence selection gradients&lt;div style="display: inline;" class="articleText"&gt;&lt;p&gt;&lt;/p&gt; &lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-184220362530548405?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2008.04.028' title='High-resolution NMR spectra in inhomogeneous fields utilizing the CRAZED sequence without coherence selection gradients'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/184220362530548405/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=184220362530548405&amp;isPopup=true' title='2 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/184220362530548405'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/184220362530548405'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/05/high-resolution-nmr-spectra-in.html' title='High-resolution NMR spectra in inhomogeneous fields utilizing the CRAZED sequence without coherence selection gradients'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>2</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1490423473341336963</id><published>2008-02-28T00:09:00.001-06:00</published><updated>2008-02-28T00:12:25.725-06:00</updated><title type='text'>Numerical simulations of motion-insensitive diffusion imaging based on the distant dipolar field effects</title><content type='html'>Tao Lin, Huijun Sun, Zhong Chen, Rongyi You, Jianhui Zhong&lt;br /&gt;Magnetic Resonance Imaging 25 (2007) 1409–1416&lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;Diffusion weighting in MRI is commonly achieved with the pulsed-gradient spin-echo (PGSE) method. When combined with spinwarping&lt;br /&gt;image formation, this method often results in ghosts due to the sample’s macroscopic motion. It has been shown experimentally&lt;br /&gt;(Kennedy and Zhong, MRM 2004;52:1–6) that these motion artifacts can be effectively eliminated by the distant dipolar field (DDF)&lt;br /&gt;method, which relies on the refocusing of spatially modulated transverse magnetization by the DDF within the sample itself. In this report,&lt;br /&gt;diffusion-weighted images (DWIs) using both DDF and PGSE methods in the presence of macroscopic sample motion were simulated.&lt;br /&gt;Numerical simulation results quantify the dependence of signals in DWI on several key motion parameters and demonstrate that the DDF&lt;br /&gt;DWIs are much less sensitive to macroscopic sample motion than the traditional PGSE DWIs. The results also show that the dipolar&lt;br /&gt;correlation distance (dc) can alter contrast in DDF DWIs. The simulated results are in good agreement with the experimental results&lt;br /&gt;reported previously.&lt;br /&gt;D 2007 Elsevier Inc. All rights reserved.&lt;br /&gt;&lt;br /&gt;Keywords: DDF; Motion; Diffusion; Image contrast; Computer simulation&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1490423473341336963?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.mri.2007.04.011' title='Numerical simulations of motion-insensitive diffusion imaging based on the distant dipolar field effects'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1490423473341336963/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1490423473341336963&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1490423473341336963'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1490423473341336963'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2008/02/numerical-simulations-of-motion.html' title='Numerical simulations of motion-insensitive diffusion imaging based on the distant dipolar field effects'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-5481107149990144739</id><published>2007-12-12T08:53:00.000-06:00</published><updated>2007-12-12T08:59:59.410-06:00</updated><title type='text'>Functional MRI at 3T using intermolecular double-quantum coherence (iDQC) with spin-echo (SE) acquisitions</title><content type='html'>&lt;a href="http://www.springerlink.com/content/110373/?p=dc0baa91b44f40fcaedb97048e78f976&amp;amp;pi=0"&gt;&lt;/a&gt;Functional MRI at 3T using intermolecular double-quantum coherence (iDQC) with spin-echo (SE) acquisitions&lt;br /&gt;T. Gu, S. D. Kennedy, Z. Chen, K. A. Schneider and J. Zhong&lt;br /&gt;Magnetic Resonance Materials in Physics, Biology and Medicine&lt;br /&gt;Published online: 5 December 2007&lt;br /&gt;&lt;span class="AbstractHeading"&gt;&lt;br /&gt;Abstract&lt;/span&gt;&lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec1"&gt;&lt;/a&gt;                   &lt;i&gt;Object&lt;/i&gt;                     &lt;/span&gt;To reinvestigate the dependence of the signal and contrast on sequence parameters and tissue relaxation times for intermolecular double-quantum coherence (iDQC) signals, and to explore the possibility to use a spin-echo (SE)-iDQC sequence for detecting activation signals at 3T. &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec2"&gt;&lt;/a&gt;                   &lt;i&gt;Materials and methods&lt;/i&gt;                     &lt;/span&gt;Brain activations were detected in five human volunteers in a visual simulation study using a SE-iDQC sequence, in addition to a GE-iDQC and a conventional single-quantum coherence (SQC) blood-oxygenation-level-dependent (BOLD) sequence. A brain phantom was also used for some quantitative measurements. &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec3"&gt;&lt;/a&gt;                   &lt;i&gt;Results&lt;/i&gt;                     &lt;/span&gt;By choosing an optimal echo time TE (~T2) and iDQC evolution time &lt;i&gt;τ&lt;/i&gt;(~20 ms), robust brain activations were detected using the SE-iDQC sequence, in addition to the GE-iDQC and a conventional single-quantum coherence (SQC) BOLD sequence. A higher percentage signal change due to activation was observed for both the iDQC-based measurements in comparison to the conventional SQC acquisition. &lt;/div&gt;          &lt;/div&gt;          &lt;div class="AbstractSection"&gt;             &lt;div class=""&gt;&lt;span class="AbstractSectionHeading"&gt;&lt;a name="ASec4"&gt;&lt;/a&gt;                   &lt;i&gt;Conclusion&lt;/i&gt;                     &lt;/span&gt;Even though a phenomenological analysis consistent with the experimental results was provided, a detailed model is still needed for the contrast mechanism at microscopic level to guide potential applications of brain functional imaging based on the SE-iDQC. &lt;/div&gt;          &lt;/div&gt;              &lt;p class="Keyword"&gt;&lt;span class="KeywordHeading"&gt;Keywords  &lt;/span&gt;fMRI - Intermolecular double-quantum coherence (iDQC) - Distant dipolar field (DDF) - Spin echo (SE)&lt;/p&gt;&lt;br /&gt;Thanks to Andreas Schaefer for sending...cac&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-5481107149990144739?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1007/s10334-007-0093-z' title='Functional MRI at 3T using intermolecular double-quantum coherence (iDQC) with spin-echo (SE) acquisitions'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/5481107149990144739/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=5481107149990144739&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5481107149990144739'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5481107149990144739'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/12/functional-mri-at-3t-using.html' title='Functional MRI at 3T using intermolecular double-quantum coherence (iDQC) with spin-echo (SE) acquisitions'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-9000146855813238577</id><published>2007-10-24T17:53:00.000-05:00</published><updated>2007-10-24T17:55:58.452-05:00</updated><title type='text'>Enhancement of magnetization transfer effects by inter-molecular multiple quantum filtered NMR</title><content type='html'>&lt;p&gt;&lt;strong&gt;Uzi Eliav&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;amp;_udi=B6WJX-4PSC2CM-1&amp;amp;_user=10&amp;amp;_coverDate=09%2F28%2F2007&amp;amp;_rdoc=14&amp;amp;_fmt=summary&amp;amp;_orig=browse&amp;amp;_srch=doc-info%28%23toc%236890%239999%23999999999%2399999%23FLA%23display%23Articles%29&amp;amp;_cdi=6890&amp;amp;_sort=d&amp;amp;_docanchor=&amp;amp;_ct=45&amp;amp;_acct=C000050221&amp;amp;_version=1&amp;amp;_urlVersion=0&amp;amp;_userid=10&amp;amp;md5=939dc94203d816a82d7e23fb3c8658a4#implicit0"&gt;&lt;sup&gt;a&lt;/sup&gt;&lt;/a&gt; and Gil Navon&lt;a name="bcor1"&gt;&lt;/a&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;amp;_udi=B6WJX-4PSC2CM-1&amp;amp;_user=10&amp;amp;_coverDate=09%2F28%2F2007&amp;amp;_rdoc=14&amp;amp;_fmt=summary&amp;amp;_orig=browse&amp;amp;_srch=doc-info%28%23toc%236890%239999%23999999999%2399999%23FLA%23display%23Articles%29&amp;amp;_cdi=6890&amp;amp;_sort=d&amp;amp;_docanchor=&amp;amp;_ct=45&amp;amp;_acct=C000050221&amp;amp;_version=1&amp;amp;_urlVersion=0&amp;amp;_userid=10&amp;amp;md5=939dc94203d816a82d7e23fb3c8658a4#cor1"&gt;&lt;sup&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/REcor.gif" alt="Corresponding Author Contact Information" border="0" /&gt;&lt;/sup&gt;&lt;/a&gt;&lt;sup&gt;, &lt;/sup&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;amp;_udi=B6WJX-4PSC2CM-1&amp;amp;_user=10&amp;amp;_coverDate=09%2F28%2F2007&amp;amp;_rdoc=14&amp;amp;_fmt=summary&amp;amp;_orig=browse&amp;amp;_srch=doc-info%28%23toc%236890%239999%23999999999%2399999%23FLA%23display%23Articles%29&amp;amp;_cdi=6890&amp;amp;_sort=d&amp;amp;_docanchor=&amp;amp;_ct=45&amp;amp;_acct=C000050221&amp;amp;_version=1&amp;amp;_urlVersion=0&amp;amp;_userid=10&amp;amp;md5=939dc94203d816a82d7e23fb3c8658a4#implicit0"&gt;&lt;sup&gt;a&lt;/sup&gt;&lt;/a&gt;&lt;sup&gt;, &lt;/sup&gt;&lt;a href="mailto:navon@post.tau.ac.il"&gt;&lt;sup&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/REemail.gif" alt="E-mail The Corresponding Author" border="0" /&gt;&lt;/sup&gt;&lt;/a&gt; &lt;/strong&gt;   &lt;br /&gt;&lt;a name="implicit0"&gt;&lt;/a&gt;&lt;sup&gt;a&lt;/sup&gt;School of Chemistry, Tel Aviv University, Ramat Aviv, Tel Aviv 69978, Israel   &lt;br /&gt; Received 10 May 2007.  Available online 28 September 2007.   &lt;br /&gt;&lt;br /&gt;&lt;/p&gt;&lt;div class="artAbs"&gt; &lt;h3 class="h3"&gt;Abstract&lt;/h3&gt;&lt;p style="text-align: justify;"&gt;There are a number of methods that give MRI contrasts based on changes of the water &lt;i&gt;M&lt;/i&gt;&lt;sub&gt;&lt;i&gt;z&lt;/i&gt;&lt;/sub&gt; magnetization as a result of magnetization transfer to macromolecules. In the present work we report that a combination of these methods with inter-molecular multiple quantum coherences (iMQC) gives enhanced effects. For the magnetization transfer contrast (MTC) method an effect of (&lt;i&gt;M&lt;/i&gt;&lt;sub&gt;&lt;i&gt;z&lt;/i&gt;&lt;/sub&gt;/&lt;i&gt;M&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;) becomes (&lt;i&gt;M&lt;/i&gt;&lt;sub&gt;&lt;i&gt;z&lt;/i&gt;&lt;/sub&gt;/&lt;i&gt;M&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;)&lt;sup&gt;&lt;i&gt;l&lt;/i&gt;&lt;/sup&gt; where &lt;i&gt;l&lt;/i&gt; is the rank of the tensors constituting the iMQC. A similar trend was found upon combining iMQC with the Goldman–Shen experiment. It is pointed out that the method is general for all magnetization transfer methods, including the nuclear Overhauser effect. &lt;/p&gt;&lt;/div&gt;&lt;br /&gt;&lt;div class="art"&gt;&lt;p&gt; &lt;strong&gt;Keywords: &lt;/strong&gt;iMQC; Intermolecular dipolar interaction; Magnetization transfer; MTC; Goldman–Shen     &lt;/p&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-9000146855813238577?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2007.09.017' title='Enhancement of magnetization transfer effects by inter-molecular multiple quantum filtered NMR'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/9000146855813238577/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=9000146855813238577&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/9000146855813238577'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/9000146855813238577'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/10/enhancement-of-magnetization-transfer.html' title='Enhancement of magnetization transfer effects by inter-molecular multiple quantum filtered NMR'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-94749582922170320</id><published>2007-10-12T05:41:00.000-05:00</published><updated>2007-10-12T05:50:09.794-05:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='ddf'/><category scheme='http://www.blogger.com/atom/ns#' term='nmr'/><category scheme='http://www.blogger.com/atom/ns#' term='iMQC'/><title type='text'>NMR Time Reversal as a Probe of Incipient Turbulent Spin Dynamics</title><content type='html'>&lt;h4 class="abs-title"&gt;&lt;/h4&gt;     NMR Time Reversal as a Probe of Incipient Turbulent Spin Dynamics&lt;br /&gt;M. E. Hayden,1 E. Baudin,2 G. Tastevin,2 and P. J. Nacher2&lt;br /&gt;&lt;br /&gt;1Physics Department, Simon Fraser University, 8888 University Drive, Burnaby BC, Canada V5A 1S6&lt;br /&gt;2Laboratoire Kastler Brossel, Ecole Normale Supérieure; CNRS; UPMC; 24 rue Lhomond, F75005 Paris, France&lt;br /&gt;    Phys. Rev. Lett. &lt;b&gt;99&lt;/b&gt;, 137602 (2007)       &lt;br /&gt;(Received 23 April 2007; published 27 September 2007)&lt;div id="abs-content-wrap"&gt;&lt;div id="abs-txt"&gt;&lt;p class="abs-history"&gt;&lt;/p&gt;                 &lt;p class="abstract"&gt;We&lt;sup&gt; &lt;/sup&gt;demonstrate time reversal of nuclear spin dynamics in highly magnetized&lt;sup&gt; &lt;/sup&gt;dilute liquid &lt;sup&gt;3&lt;/sup&gt;He-&lt;sup&gt;4&lt;/sup&gt;He mixtures through effective inversion of long-range dipolar&lt;sup&gt; &lt;/sup&gt;interactions. These experiments, which involve using magic sandwich NMR pulse&lt;sup&gt; &lt;/sup&gt;sequences to generate spin echoes, probe the spatiotemporal development of&lt;sup&gt; &lt;/sup&gt;turbulent spin dynamics and promise to serve as a versatile&lt;sup&gt; &lt;/sup&gt;tool for the study and control of dynamic magnetization instabilities.&lt;sup&gt; &lt;/sup&gt;We also show that a repeated magic sandwich pulse sequence&lt;sup&gt; &lt;/sup&gt;can be used to dynamically stabilize modes of nuclear precession&lt;sup&gt; &lt;/sup&gt;that are otherwise intrinsically unstable. To date, we have extended&lt;sup&gt; &lt;/sup&gt;the effective precession lifetimes of our magnetized samples by more&lt;sup&gt; &lt;/sup&gt;than three orders of magnitude.&lt;/p&gt;(Thanks to Louis Bouchard for sending...Curt)&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-94749582922170320?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1103/PhysRevLett.99.137602' title='NMR Time Reversal as a Probe of Incipient Turbulent Spin Dynamics'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/94749582922170320/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=94749582922170320&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/94749582922170320'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/94749582922170320'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/10/nmr-time-reversal-as-probe-of-incipient.html' title='NMR Time Reversal as a Probe of Incipient Turbulent Spin Dynamics'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1758480529555260817</id><published>2007-09-28T12:42:00.000-05:00</published><updated>2007-09-28T12:46:47.761-05:00</updated><title type='text'>Functional contrast based on intermolecular double-quantum coherences: Influence of the correlation distance</title><content type='html'>&lt;table width="100%"&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td&gt;Andreas Schäfer&lt;sup&gt;&lt;span style="font-size:-1;"&gt; 1 2&lt;/span&gt;&lt;/sup&gt;, Harald E. Möller&lt;sup&gt;&lt;span style="font-size:-1;"&gt; 1&lt;/span&gt;&lt;span style="font-size:-1;"&gt; *&lt;/span&gt;&lt;/sup&gt;&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td&gt;&lt;sup&gt;&lt;span style="font-size:-1;"&gt;1&lt;/span&gt;&lt;/sup&gt;Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany&lt;br /&gt;&lt;sup&gt;&lt;span style="font-size:-1;"&gt;2&lt;/span&gt;&lt;/sup&gt;University of Nottingham, School of Physics and Astronomy, Sir Peter Mansfield Magnetic Resonance Centre, University Park, Nottingham, United Kingdom&lt;br /&gt;&lt;/td&gt;&lt;/tr&gt;&lt;tr&gt;&lt;td&gt;&lt;b&gt;email:&lt;/b&gt; Harald E. Möller (&lt;a href="mailto:moeller@cbs.mpg.de"&gt;moeller@cbs.mpg.de&lt;/a&gt;)&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;p&gt;&lt;sup&gt;&lt;span style="font-size:-1;"&gt;*&lt;/span&gt;&lt;/sup&gt;Correspondence to Harald E. Möller, Max Planck Institute for Human Cognitive and Brain Sciences, Stephanstr. 1a, 04103 Leipzig, Germany&lt;/p&gt;&lt;script language="JavaScript"&gt;setDOI("ADOI=10.1002/mrm.21406")&lt;/script&gt;&lt;table border="0" width="100%"&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td class="mainSectionHeader"&gt;&lt;a name="keywords"&gt;Keywords&lt;/a&gt;&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;table&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td&gt;BOLD contrast • correlation distance • distant dipolar field • intermolecular double-quantum coherence (iDQC)&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;table border="0" width="100%"&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td class="mainSectionHeader"&gt;&lt;a name="abstract"&gt;Abstract&lt;/a&gt;&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;table border="0" width="100%"&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td&gt;A functional MRI (fMRI) study with visual stimulation of healthy subjects was performed at 3T exploiting intermolecular double-quantum coherences. The correlation distance, &lt;i&gt;d&lt;/i&gt;&lt;sub&gt;&lt;i&gt;c&lt;/i&gt;&lt;/sub&gt;, was varied between 60 and 300 &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/mu.gif" align="absbottom" border="0" /&gt;m for different evolution times, &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/tau.gif" border="0" /&gt;. Robust activation was obtained in all experiments with average signal changes (&lt;span style="color:#999999;"&gt;[bar &lt;/span&gt;&lt;img src="http://www3.interscience.wiley.com/giflibrary/12/Delta.gif" border="0" /&gt;&lt;i&gt;S&lt;/i&gt;&lt;sub&gt;&lt;i&gt;2&lt;/i&gt;&lt;/sub&gt;&lt;span style="color:#999999;"&gt; ]&lt;/span&gt;) = 8.4 ± 0.7% and 9.4 ± 0.8% for &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/tau.gif" border="0" /&gt; = 15 and 20 ms, respectively) exceeding those normally associated with conventional blood oxygen level-dependent (BOLD) fMRI. Relaxation-rate changes (&lt;img src="http://www3.interscience.wiley.com/giflibrary/12/Delta.gif" border="0" /&gt;&lt;i&gt;R&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt; = 0.33 ± 0.36 s&lt;sup&gt;-1&lt;/sup&gt; and &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/Delta.gif" border="0" /&gt;&lt;i&gt;R&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt;* = 0.77 ± 0.54 s&lt;sup&gt;-1&lt;/sup&gt;) were similar to those commonly obtained for the extravascular BOLD effect. The number of activated voxels increased with increasing &lt;i&gt;d&lt;/i&gt;&lt;sub&gt;&lt;i&gt;c&lt;/i&gt;&lt;/sub&gt; until a plateau was reached at &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/ap.gif" border="0" /&gt;120 &lt;img src="http://www3.interscience.wiley.com/giflibrary/12/mu.gif" align="absbottom" border="0" /&gt;m. Similar trends were observed for the activation-induced percent signal change and for the maximal &lt;i&gt;Z&lt;/i&gt;-scores. These effects were quantitatively explained by a reduced sensitivity at short &lt;i&gt;d&lt;/i&gt;&lt;sub&gt;&lt;i&gt;c&lt;/i&gt;&lt;/sub&gt; due to increasing signal attenuation related to diffusion and an increasing amount of signal fluctuations in the fMRI time series due to imperfect suppression of unwanted coherence pathways. Consistent indications of a preferential selection of susceptibility changes in blood vessels of a particular size were not obtained. Magn Reson Med 58:696-704, 2007. © 2007 Wiley-Liss, Inc.&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;hr align="left" size="1" width="25%"&gt;Received: 16 March 2007; Revised: 30 July 2007; Accepted: 6 August 2007&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1758480529555260817?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www3.interscience.wiley.com/cgi-bin/abstract/116323867/ABSTRACT' title='Functional contrast based on intermolecular double-quantum coherences: Influence of the correlation distance'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1758480529555260817/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1758480529555260817&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1758480529555260817'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1758480529555260817'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/09/functional-contrast-based-on.html' title='Functional contrast based on intermolecular double-quantum coherences: Influence of the correlation distance'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-301104250048939538</id><published>2007-08-30T10:40:00.000-05:00</published><updated>2007-08-30T11:35:22.776-05:00</updated><title type='text'>Assessing signal enhancement in distant dipolar field-based sequences</title><content type='html'>&lt;span class="txt; !important"&gt;Wilson Barros Jr., Daniel F. Gochberg and John C. Gore&lt;br /&gt;&lt;/span&gt;&lt;br /&gt;Abstract&lt;br /&gt;The possibility of improving the signal-to-noise efficiency of NMR signal refocused by long-range dipolar interactions has been discussed recently [Branca et al., JMR 187 (2007) 38-43]. For systems where T1&lt;&lt; T2, by including an extra radio-frequency pulse in a standard CRAZED sequence, it is possible to increase the available signal by exploiting its sensitivity to T1 relaxation. Here, we use analytical calculations to investigate the source of this improved signal and determine the maximum enhancement provided by the method.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-301104250048939538?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2007.08.015' title='Assessing signal enhancement in distant dipolar field-based sequences'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/301104250048939538/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=301104250048939538&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/301104250048939538'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/301104250048939538'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/08/assessing-signal-enhancement-in-distant.html' title='Assessing signal enhancement in distant dipolar field-based sequences'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4485920931825433898</id><published>2007-08-30T10:37:00.000-05:00</published><updated>2007-08-30T11:35:50.516-05:00</updated><title type='text'>Apparent Longitudinal Relaxation in Solutions with Intermolecular Dipolar Interactions and Slow Chemical Exchange</title><content type='html'>&lt;span class="txt; !important"&gt;Shengchun Zhang, Xiaoqin Zhu, Zhong Chen, Shuhui Cai and Jianhui Zhong&lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;A modified CRAZED sequence with selective inversion before excitation was designed to investigate the longitudinal relaxation under the effects of slow chemical exchange and distant dipolar interactions in highly polarized spin systems. Analytical expressions for the apparent longitudinal relaxation time of such systems were derived from a combination of the dipolar field theory and product operator formalism. The result shows that the signal intensity follows a multi-exponential function of the inversion-recovery time. Experimental results support the theoretical predictions.&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4485920931825433898?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2007.08.038' title='Apparent Longitudinal Relaxation in Solutions with Intermolecular Dipolar Interactions and Slow Chemical Exchange'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4485920931825433898/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4485920931825433898&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4485920931825433898'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4485920931825433898'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/08/apparent-longitudinal-relaxation-in.html' title='Apparent Longitudinal Relaxation in Solutions with Intermolecular Dipolar Interactions and Slow Chemical Exchange'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4028258419098754480</id><published>2007-08-23T13:33:00.000-05:00</published><updated>2007-08-23T13:37:44.900-05:00</updated><title type='text'>Finite Element Formulation of the Bloch Equations with Dipolar Field Effects</title><content type='html'>&lt;a href="http://arxiv.org/find/physics/1/au:+Bouchard_L/0/1/0/all/0/1"&gt;&lt;/a&gt;Louis-S. Bouchard&lt;br /&gt;(Submitted on 24 Jun 2007)&lt;br /&gt;arXiv.org&lt;div class="dateline"&gt;&lt;br /&gt;&lt;/div&gt;A Galerkin finite element (FEM) formulation for the Bloch equations with dipolar field is presented which makes possible the derivation of weak solutions to the Bloch equations. The FEM formulation has the advantage that the equations of motion are local in real space, eliminating the global truncation errors associated with calculations of the dipolar field in Fourier space. The dipolar field and other geometric parameters are calculated only once, before the simulation, and used as an initial condition rather than re-calculated at every time step of some numerical integration.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4028258419098754480?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://arxiv.org/abs/0706.3540' title='Finite Element Formulation of the Bloch Equations with Dipolar Field Effects'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4028258419098754480/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4028258419098754480&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4028258419098754480'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4028258419098754480'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/08/finite-element-formulation-of-bloch.html' title='Finite Element Formulation of the Bloch Equations with Dipolar Field Effects'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-4113831150996714232</id><published>2007-04-30T23:46:00.000-05:00</published><updated>2007-05-01T09:43:38.363-05:00</updated><title type='text'>Numerical simulations of contribution of chemical shift in novel magnetic resonance imaging</title><content type='html'>&lt;p class="AuthorGroup"&gt;&lt;/p&gt;Huijun Sun, Tao Lin, Shuhui Cai and Zhong Chen&lt;br /&gt;Lecture Notes in Computer ScienceVolume 4222/2006&lt;br /&gt;Advances in Natural Computation&lt;br /&gt;&lt;br /&gt;&lt;p class="AuthorGroup"&gt;&lt;b&gt;Abstract&lt;/b&gt;&lt;br /&gt;Contribution of chemical shift to intermolecular multiple-quantum coherence (iMQC) imaging signals in two-component systems was simulated and discussed using an efficient numerical algorithm based on the Bloch equations with an additional nonlinear term describing distant dipolar field. Numerical simulation switches back and forth between real and Fourier spaces to handle dipolar field effects in three-dimensional sample. The iMQC signals of each component of two-component systems can be obtained respectively when the second pulse of the CRAZED pulse sequence is selective. Simulation results show that chemical shift provides an edge detection method to regions containing spins with chemical shift offset and selected by the second RF pulse, and different gray value is related to different chemical shift in detected regions. These results indicate that chemical shift may provide new imaging information helpful for iMQC magnetic resonance imaging. &lt;/p&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-4113831150996714232?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1007/11881223_46' title='Numerical simulations of contribution of chemical shift in novel magnetic resonance imaging'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/4113831150996714232/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=4113831150996714232&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4113831150996714232'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/4113831150996714232'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/04/numerical-simulations-of-contribution.html' title='Numerical simulations of contribution of chemical shift in novel magnetic resonance imaging'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-7458957851461667801</id><published>2007-04-30T23:36:00.000-05:00</published><updated>2007-05-01T09:38:06.487-05:00</updated><title type='text'>Multiple quantum correlated spectroscopy revamped by asymmetric z-gradient echo detection signal intensity as a function of the read pulse flip angle</title><content type='html'>&lt;dl&gt;&lt;dd&gt;&lt;/dd&gt; &lt;/dl&gt;Bin Jiang, Huili Liu, China    Maili Liu, Chaohui Ye, and China    Xi-an Mao&lt;br /&gt;J. Chem. Phys. 126, 054502 (2007)   &lt;p&gt;   &lt;/p&gt;&lt;p&gt;   (Received 28 August 2006; accepted 5 December 2006; published online 1 February 2007)       &lt;/p&gt;  Heteronuclear&lt;sup&gt; &lt;/sup&gt;multiple quantum (&lt;i&gt;n&lt;/i&gt;=±0 and &lt;i&gt;n&lt;/i&gt;=±2) correlated spectroscopy revamped by asymmetric&lt;sup&gt; &lt;/sup&gt;&lt;i&gt;z&lt;/i&gt;-gradient echo detection (CRAZED) experiments were performed on the spins&lt;sup&gt; &lt;/sup&gt;&lt;sup&gt;31&lt;/sup&gt;P and &lt;sup&gt;1&lt;/sup&gt;H in a H&lt;sub&gt;3&lt;/sub&gt;PO&lt;sub&gt;4&lt;/sub&gt; solution in order to&lt;sup&gt; &lt;/sup&gt;determine the optimum flip angle for the read pulse. It&lt;sup&gt; &lt;/sup&gt;has been shown that for the negative quantum signals, the&lt;sup&gt; &lt;/sup&gt;maximum signals appear at &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;=0, and for the positive quantum&lt;sup&gt; &lt;/sup&gt;signals, the maximum signals appear at &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;=&lt;img src="http://scitation.aip.org/stockgif3/pgr.gif" alt="pi" align="bottom" border="0" /&gt;. The CRAZED signals&lt;sup&gt; &lt;/sup&gt;were compared to the single quantum signals in two-pulse two-gradient&lt;sup&gt; &lt;/sup&gt;experiments. It is found that the CRAZED signals can also&lt;sup&gt; &lt;/sup&gt;be distinguished into gradient echoes and spin echoes. The gradient-echo-type&lt;sup&gt; &lt;/sup&gt;CRAZED signal requires &lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;=0 and the spin-echo-type CRAZED signal requires&lt;sup&gt; &lt;/sup&gt;&lt;img src="http://scitation.aip.org/stockgif3/bgr.gif" alt="beta" align="middle" border="0" /&gt;=&lt;img src="http://scitation.aip.org/stockgif3/pgr.gif" alt="pi" align="bottom" border="0" /&gt; for maximum echo intensities, in the same way as&lt;sup&gt; &lt;/sup&gt;in single quantum experiments.   ©2007 &lt;i&gt;American Institute of Physics&lt;/i&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-7458957851461667801?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1063/1.2429657' title='Multiple quantum correlated spectroscopy revamped by asymmetric z-gradient echo detection signal intensity as a function of the read pulse flip angle'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/7458957851461667801/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=7458957851461667801&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7458957851461667801'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7458957851461667801'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/04/multiple-quantum-correlated.html' title='Multiple quantum correlated spectroscopy revamped by asymmetric z-gradient echo detection signal intensity as a function of the read pulse flip angle'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-7109648238572531258</id><published>2007-04-30T23:31:00.000-05:00</published><updated>2007-05-01T09:42:01.273-05:00</updated><title type='text'>Simultaneous acquisition and effective separation of intermolecular multiple-quantum signals of different orders</title><content type='html'>&lt;p&gt;&lt;strong&gt;&lt;/strong&gt;&lt;/p&gt;Xiaoqin Zhu, Song Chen, Zhong Chen, Shuhui Cai and Jianhui Zhong&lt;br /&gt;Chemical Physics Letters  &lt;br /&gt;               Volume 438, Issues 4-6,    20 April 2007,   Pages 308-314        &lt;br /&gt;                &lt;br /&gt;Abstract&lt;br /&gt;A three-pulse sequence was designed to simultaneously acquire intermolecular multiple-quantum coherence (iMQC) signals of coherence order &lt;i&gt;n&lt;/i&gt; = 2, 1, 0, −1, −2. Analytical expressions were derived from modified Bloch equations. Signal of a specific order was obtained by optimal combinations of data from different acquisition steps. This allows a time saving of 5/7 compared to the phase cycling designs targeted for individual coherence orders. The method also results in pure iMQC signal of all the above five orders which are insensitive to radio-frequency flip angle errors, in contrast to some previous methods. Theoretical predictions are supported by the experimental observations and numerically simulated results.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-7109648238572531258?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2007.02.059' title='Simultaneous acquisition and effective separation of intermolecular multiple-quantum signals of different orders'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/7109648238572531258/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=7109648238572531258&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7109648238572531258'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/7109648238572531258'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/04/simultaneous-acquisition-and-effective.html' title='Simultaneous acquisition and effective separation of intermolecular multiple-quantum signals of different orders'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-3582169428158415234</id><published>2007-04-30T23:23:00.000-05:00</published><updated>2007-05-01T09:40:59.079-05:00</updated><title type='text'>Magnetic resonance microscopic imaging based on high-order intermolecular multiple-quantum coherences</title><content type='html'>&lt;p&gt;&lt;strong&gt;&lt;/strong&gt;&lt;/p&gt;Jee-Hyun Cho, Sangdoo Ahn, Chulhyun Lee, Kwan Soo Hong, Kee-Choo Chung, Suk-Kyu Chang, Chaejoon Cheong and Warren S. Warren&lt;br /&gt;Magnetic Resonance Imaging   &lt;br /&gt;          Article in Press, Corrected Proof&lt;br /&gt;  &lt;div class="art"&gt;&lt;p&gt;&lt;span class="h3"&gt;Abstract&lt;/span&gt;&lt;/p&gt;&lt;p&gt;Most imaging studies using intermolecular multiple-quantum coherences (iMQCs) have focused on the two-spin dipolar interactions — zero and double quantum coherences. Here, we report the results of various experimental studies to assess the feasibility of magnetic resonance microscopy with high-order iMQCs in model systems at 7 and 14 T. Experimental results demonstrated that the iMQC microscopic images with high coherence orders are readily observable at high field and have unique contrast depending on the sample microstructure and coherence order. &lt;/p&gt;&lt;p&gt; &lt;strong&gt;Keywords: &lt;/strong&gt;Intermolecular multiple-quantum coherence; iTQC; iQQC; MR microscopy  &lt;br /&gt;&lt;/p&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-3582169428158415234?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://linkinghub.elsevier.com/retrieve/pii/S0730725X06002876' title='Magnetic resonance microscopic imaging based on high-order intermolecular multiple-quantum coherences'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/3582169428158415234/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=3582169428158415234&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/3582169428158415234'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/3582169428158415234'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/04/magnetic-resonance-microscopic-imaging.html' title='Magnetic resonance microscopic imaging based on high-order intermolecular multiple-quantum coherences'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-5189805276154517736</id><published>2007-04-28T22:30:00.000-05:00</published><updated>2007-04-28T22:41:10.878-05:00</updated><title type='text'>Signal enhancement in CRAZED experiments</title><content type='html'>&lt;span class="articleTitle"&gt; &lt;p&gt;&lt;/p&gt;&lt;/span&gt;&lt;span style="font-weight: bold;"&gt;Signal enhancement in CRAZED experiments&lt;/span&gt;&lt;br /&gt;Rosa T. Branca, Gigi Galiana and Warren S. Warren&lt;br /&gt;&lt;span style="font-style: italic;"&gt;Journal of Magnetic Resonance&lt;/span&gt;  &lt;br /&gt;         Article in Press, Corrected Proof&lt;br /&gt;&lt;br /&gt;Many of the promising applications of the CRAZED (COSY Revamped with Asymmetric Z-gradient Echo Detection) experiments are in biomedical and clinical technologies. In tissue, however, signal from the typical CRAZED experiment is largely limited by transverse relaxation. When relaxation is included, the maximum achievable signal from a prototypical CRAZED sequence, in the linear regime, is proportional to T2/τd. This means that for samples with a short T2, as encountered in vivo, signals from intermolecular multiple-quantum coherences (iMQCs) reach very diminished signal intensities. While relaxation is generally regarded as a fundamental constraint, we show here that when T2 is short but T1 is long, as in tissue, there are simple sequence modifications that can increase signal beyond the T2 limit. To better utilize the available signal intensity from iMQCs we propose a method to substitute part of the transverse magnetization with the longitudinally modulated magnetization. In this paper we show, with both simulations and experimental results, that in the presence of strong transverse relaxation the standard CRAZED scheme is not the optimal method for observing iMQCs, and can be improved upon with simple modifications.&lt;br /&gt;&lt;br /&gt;Keywords: CRAZED; iZQC; iDQC; Dipolar demagnetization time&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-5189805276154517736?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2007.02.017' title='Signal enhancement in CRAZED experiments'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/5189805276154517736/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=5189805276154517736&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5189805276154517736'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/5189805276154517736'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/04/signal-enhancement-in-crazed.html' title='Signal enhancement in CRAZED experiments'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-8798675035480520812</id><published>2007-03-27T14:43:00.000-05:00</published><updated>2007-03-27T14:46:27.656-05:00</updated><title type='text'>Gradient-echo and CRAZED imaging for minute detection of Alzheimer plaques in an APPV717I × ADAM10-dn mouse model</title><content type='html'>Cornelius Faber, Benjamin Zahneisen, Frank Tippmann, Anja Schroeder, Falk Fahrenholz&lt;br /&gt;Magnetic Resonance in Medicine&lt;br /&gt;Published Online: 27 Mar 2007&lt;br /&gt;&lt;br /&gt;Different strategies to visualize amyloid plaques with MRI at 17.6 Tesla were investigated in a novel mouse model of Alzheimer's disease (AD). Large iron-containing plaques were observed in the thalamus, but cortical plaques did not show iron deposits. Plaques in the thalamus were visualized in vivo with the use of low-resolution, 3D gradient-echo (GRE) imaging in 82 s, and with 94-&lt;img src="http://www3.interscience.wiley.com/giflibrary/12/mu.gif" align="absbottom" border="0" /&gt;m resolution in 34 min. The feasibility of obtaining bright contrast from plaques using the COSY revamped with asymmetric &lt;i&gt;z&lt;/i&gt;-GRE detection (CRAZED) technique was investigated in experiments on fixed brains. The original CRAZED approach provided reduced signal near the plaques (similarly to GRE imaging) and additionally emphasized small structures in the brain. In CRAZED images acquired with mismatched gradients, elevated signal near the plaques was obtained, while background signal was suppressed almost to the noise level. Bright-contrast images were acquired in 2.6 min with the use of a 2D GRE sequence with slightly mismatched slice refocusing gradients. For future detection of plaques in patients, such bright-contrast visualization protocols may be of particular value when contrast agents that allow labeling of early plaques with iron oxide nanoparticles become available. Magn Reson Med 57:696-703, 2007. © 2007 Wiley-Liss, Inc.&lt;br /&gt;&lt;br /&gt;&lt;pre wrap=""&gt;&lt;/pre&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-8798675035480520812?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21201' title='Gradient-echo and CRAZED imaging for minute detection of Alzheimer plaques in an APPV717I × ADAM10-dn mouse model'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/8798675035480520812/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=8798675035480520812&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8798675035480520812'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/8798675035480520812'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/03/gradient-echo-and-crazed-imaging-for.html' title='Gradient-echo and CRAZED imaging for minute detection of Alzheimer plaques in an APPV717I × ADAM10-dn mouse model'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-2939848846817638946</id><published>2007-03-15T23:16:00.000-05:00</published><updated>2007-05-01T10:03:55.441-05:00</updated><title type='text'>Indirect detection of NMR via geometry-dependent dipolar fields, revisited</title><content type='html'>&lt;span class="txt; !important"&gt;Journal of Magnetic Resonance&lt;br /&gt;&lt;i&gt;&lt;b&gt;&lt;span style="color: rgb(255, 0, 0);"&gt;In Press, Accepted Manuscript&lt;/span&gt;&lt;/b&gt;&lt;/i&gt;, &lt;i&gt;Available online 1 March 2007&lt;/i&gt;,&lt;br /&gt;Wei Dong and CA. Meriles&lt;br /&gt;&lt;br /&gt;&lt;/span&gt; &lt;div style="text-align: left;"&gt;&lt;span class="txt; !important"&gt;We explore the dipolar interactions between two separate nuclear spin ensembles&lt;/span&gt;&lt;span class="txt; !important"&gt; in a mixture containing oil and water. Here we expand initial results (C.A. Meriles and&lt;/span&gt;&lt;span class="txt; !important"&gt; W. Dong, J. Magn. Reson. 181, 331 (2006)) to the case in which both systems have the&lt;/span&gt;&lt;span class="txt; !important"&gt; shape of flat, stacked disks. We find that -  spite of the strong inhomogeneity of the&lt;/span&gt;&lt;span class="txt; !important"&gt;coupling dipolar field - the signal encoded in one of the components can be made&lt;/span&gt;&lt;span class="txt; !important"&gt; approximately proportional to the magnetization in the other. This allows us to use one of&lt;/span&gt;&lt;span class="txt; !important"&gt; these systems as a ‘sensor’ to indirectly reconstruct the resonance spectrum or to&lt;/span&gt;&lt;span class="txt; !important"&gt; determine the relaxation time of the ‘sample’ system. In the regime in which dipolar&lt;/span&gt;&lt;span class="txt; !important"&gt; interactions are sufficiently strong, our method can be set to scale-up weaker signals in a&lt;/span&gt;&lt;span class="txt; !important"&gt; non-linear fashion, which, potentially, could allow one to introduce contrast or to&lt;/span&gt;&lt;span class="txt; !important"&gt; improve detection sensitivity of less magnetized samples.&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-2939848846817638946?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2007.02.012' title='Indirect detection of NMR via geometry-dependent dipolar fields, revisited'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/2939848846817638946/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=2939848846817638946&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2939848846817638946'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/2939848846817638946'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/03/indirect-detection-of-nmr-via-geometry.html' title='Indirect detection of NMR via geometry-dependent dipolar fields, revisited'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-1137408350512158817</id><published>2007-02-09T18:37:00.000-06:00</published><updated>2007-02-09T18:36:14.849-06:00</updated><title type='text'>Theoretical studies of the effect of the dipolar field in multiple spin-echo sequences with refocusing pulses of finite duration</title><content type='html'>Chung Ki Wong, Scott D. Kennedy, Edmund Kwok and Jianhui Zhong&lt;br /&gt;&lt;br /&gt;Journal of Magnetic Resonance                                       &lt;br /&gt;Article in Press,         Corrected Proof &lt;br /&gt;&lt;br /&gt;&lt;p&gt;&lt;/p&gt;It has been observed recently that the finite duration of refocusing rf pulses in a multiecho acquisition of the signal formed under the influence of the dipolar field leads to significant signal attenuation [S. Kennedy, Z. Chen, C.K. Wong, E.W.-C. Kwok, J. Zhong, Investigation of multiple-echo spin-echo signal acquisition under distant dipole–dipole interactions, Proc. Int. Soc. Magn. Reson. Med. 13 (2005) 2288]. Hereto, we quantify the phenomenon by evaluating analytically the influences of both the distant dipolar field (DDF) and transverse relaxation T2 on the magnetization in a multiecho pulse sequence based on correlation spectroscopy revamped by asymmetric z-gradient echo detection (CRAZED). Analytic expressions for the magnetization were obtained, which demonstrate explicitly the origin of rephased signal in the presence of the finite π pulses in the multiecho train. The expressions also explain the effects of the DDF and T2 during the refocusing pulses on the signal strength, and show the substantial signal dependence on the phase of the rf pulses. We show that when the DDF effect during the pulse is canceled, the signal rises primarily during the free evolution time in the acquisition period. This elucidates the signal attenuation when the rf pulses cover a significant proportion of time in the sequence. In addition, we performed an optimization on the number of refocusing pulses that maximizes the total acquired signal using parameters for water, brain white matter, and muscle. We found that maximal signal-to-noise ratio is obtained when the pulse duration approximately equals the free evolution time in the samples with a wide range of T2.&lt;br /&gt;&lt;br /&gt;Keywords: Distant dipolar field; Multiple spin-echo sequence; Finite pulse; Intermolecular double-quantum coherence   &lt;br /&gt;&lt;span style="font-size: smaller; font-family: Verdana;"&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-1137408350512158817?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org.floyd.lib.umn.edu/10.1016/j.jmr.2006.12.017' title='Theoretical studies of the effect of the dipolar field in multiple spin-echo sequences with refocusing pulses of finite duration'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/1137408350512158817/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=1137408350512158817&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1137408350512158817'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/1137408350512158817'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/02/theoretical-studies-of-effect-of.html' title='Theoretical studies of the effect of the dipolar field in multiple spin-echo sequences with refocusing pulses of finite duration'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-116838674729787118</id><published>2007-01-09T17:50:00.000-06:00</published><updated>2007-01-09T17:52:27.296-06:00</updated><title type='text'>Yahoo Group ddf_imqc</title><content type='html'>Here is the link to the new yahoo discussion group.&lt;br /&gt;&lt;br /&gt;This is to facillitate more interactive technical discussion on DDF and iMQC related magnetic resonance.&lt;br /&gt;&lt;br /&gt;Curt&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-116838674729787118?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://groups.yahoo.com/group/ddf_imqc' title='Yahoo Group ddf_imqc'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/116838674729787118/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=116838674729787118&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116838674729787118'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116838674729787118'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2007/01/yahoo-group-ddfimqc.html' title='Yahoo Group ddf_imqc'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-116482723460820295</id><published>2006-11-29T13:04:00.000-06:00</published><updated>2006-11-29T13:08:44.896-06:00</updated><title type='text'>Contrast Enhancement by Feedback Fields in Magnetic Resonance Imaging</title><content type='html'>&lt;p&gt;  &lt;au&gt;&lt;b&gt;Sandip Datta,&lt;/b&gt;&lt;/au&gt;  &lt;au&gt;&lt;b&gt;Susie Y. Huang, and&lt;/b&gt;&lt;/au&gt;  &lt;au&gt;&lt;b&gt;Yung-Ya Lin*&lt;/b&gt;&lt;/au&gt;  &lt;/p&gt;&lt;aff&gt;&lt;/aff&gt;&lt;p&gt;&lt;i&gt;Department of Chemistry and Biochemistry, University of California, Los Angeles, California 90095  &lt;/i&gt;&lt;/p&gt;    &lt;p&gt;&lt;i&gt;Received: January 31, 2006&lt;/i&gt;&lt;/p&gt;  &lt;p&gt;&lt;i&gt;In Final Form: April 25, 2006&lt;/i&gt;&lt;/p&gt;  &lt;abs&gt;&lt;/abs&gt;&lt;p&gt;&lt;b&gt;Abstract:&lt;/b&gt;&lt;/p&gt;  &lt;p&gt;A conceptually new approach giving rise to contrast enhancement by feedback fields in magnetic resonance  imaging is proposed, and the detailed mechanism is described. Nonlinear spin dynamics under the feedback  fields of the distant dipolar field and/or radiation damping are examined and shown to amplify contrast due  to small variations in spin density and precession frequency. Feedback-based contrast enhancement depends  on the instability of the initial magnetization configuration and is propagated by positive feedback, as shown  through numerical simulations and experimental results on simple phantom samples. On the basis of a theoretical  understanding of contrast enhancement, insight into pulse sequence design and optimal contrast attainable  under the individual and joint feedback fields is provided.  &lt;/p&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-116482723460820295?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1021/jp060658k' title='Contrast Enhancement by Feedback Fields in Magnetic Resonance Imaging'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/116482723460820295/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=116482723460820295&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116482723460820295'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116482723460820295'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/11/contrast-enhancement-by-feedback.html' title='Contrast Enhancement by Feedback Fields in Magnetic Resonance Imaging'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-116482697092689553</id><published>2006-11-29T12:59:00.000-06:00</published><updated>2006-11-29T13:03:59.516-06:00</updated><title type='text'>Direct enhancement of any solution NMR signal using the distant dipolar fields created by highly polarized and concentrated nuclear spin systems</title><content type='html'>&lt;b&gt;H. Desvaux, D.J. Marion, G. Huber, L. Dubois and P. Berthault &lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Laboratoire Structure et Dynamique par Résonance Magnétique, Service de Chimie Moléculaire,  URA CEA/CNRS 331 Claude Fréjacques, CEA/Saclay, 91191 Gif-sur-Yvette, France&lt;br /&gt;&lt;a href="mailto:hdesvaux@cea.fr" _base_href="http://www.edpsciences.org/articles/epjap/abs/2006/10/ap06124/ap06124.html"&gt;hdesvaux@cea.fr&lt;/a&gt;&lt;br /&gt;&lt;!--idline--&gt;&lt;br /&gt;(Received: 9 May 2006 / Accepted: 26 July 2006     / Published online: 6 October 2006)&lt;br /&gt;&lt;p align="left"&gt;&lt;strong&gt; Abstract &lt;/strong&gt;&lt;br /&gt;Peculiar nuclear spin systems can be polarized at a level of thousands times the value obtained at thermal equilibrium, for instance by optical pumping. When concentrated, these systems create a sizeable average dipolar field which is experienced by any nuclear spin. We propose to use these distant dipolar fields for performing a polarization transfer in the Hartmann-Hahn conditions. We report the maximum enhancement value calculated using the spin temperature approach and first theoretical insights on the polarization transfer rate. Using, as an example, dissolved laser-polarized xenon, we show that by spin-locking both xenon spins and a proton spin of a solute, the polarization of the latter is enhanced. This is obtained without the existence of chemical interaction between the two entities and with characteristic rising time not directly correlated to the proton self-relaxation time. By its generality and its non-local feature, this approach could make possible nuclear magnetic resonance spectroscopy on very dilute systems.    &lt;/p&gt;&lt;b&gt; PACS &lt;/b&gt;&lt;br /&gt;82.56.-b - Nuclear magnetic resonance.   &lt;br /&gt;76.70.-r - Magnetic double resonances and cross effects.   &lt;br /&gt;82.56.Jn - Pulse sequences in NMR.   &lt;br /&gt;32.80.Bx - Level crossing and optical pumping.   &lt;br /&gt;&lt;br /&gt;&lt;b&gt;© &lt;/b&gt;&lt;i&gt;EDP Sciences 2006&lt;/i&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-116482697092689553?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1051/epjap:2006107' title='Direct enhancement of any solution NMR signal using the distant dipolar fields created by highly polarized and concentrated nuclear spin systems'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/116482697092689553/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=116482697092689553&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116482697092689553'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116482697092689553'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/11/direct-enhancement-of-any-solution-nmr.html' title='Direct enhancement of any solution NMR signal using the distant dipolar fields created by highly polarized and concentrated nuclear spin systems'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-116364429161500742</id><published>2006-11-15T20:30:00.000-06:00</published><updated>2006-11-15T20:31:31.626-06:00</updated><title type='text'>Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)</title><content type='html'>In the CRAZED experiment (COSY revamped by asymmetric Z-gradient echo detection, Warren et al.), a spatially anisotropic magnetization distribution is created by application of a magnetic field gradient (strength G, duration τ) which in turn generates a response called the distant dipolar field (DDF). The DDF is a source of intermolecular multiple-quantum coherences (iMQC) which contain information on the distance d = π/(γGτ) between pairs of dipolar-coupled spins. Diffraction-like phenomena may result for periodically structured samples. In this study, we report the observation of diffraction owing to the DDF at 1.5 T using a clinical whole-body tomograph. Based on the semi-classical treatment of the problem by Robyr and Bowtell, diffraction conditions were obtained for a CRAZED-type pulse sequence that selects iMQC of order N. The predicted distinct difference in N = 2 and N ≠ 2 coherences, i.e., a dominant continuous course as a function of τ (N = 2) and prominent diffraction peaks otherwise, could be verified in CRAZED experiments in a periodically structured sample selecting coherence orders N = 2 and N = 3. The diffractive signal component contains information on the geometric structure of the sample. Applications of this technique may permit the detection of changes in composition and geometry of periodic structures.&lt;br /&gt;Keywords: CRAZED; Distant dipolar field (DDF); Intermolecular multiple-quantum coherence; Diffraction&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-116364429161500742?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2006.10.011' title='Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/116364429161500742/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=116364429161500742&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116364429161500742'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/116364429161500742'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/11/diffraction-like-phenomena-in-periodic.html' title='Diffraction-like phenomena in a periodic magnetization distribution at 1.5 T using the distant dipolar field (DDF)'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-115930864969935012</id><published>2006-09-26T17:05:00.000-05:00</published><updated>2006-11-15T20:34:43.323-06:00</updated><title type='text'>Fast single-gradient simultaneous measurement of D and T2 in liquids via the distant dipolar field</title><content type='html'>Wilson Barros, Jr&lt;a name="bcor1"&gt;&lt;/a&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6TFN-4KX00R3-5&amp;amp;amp;amp;amp;amp;amp;amp;_coverDate=09%2F16%2F2006&amp;_alid=456445778&amp;amp;_rdoc=1&amp;_fmt=&amp;amp;_orig=search&amp;_qd=1&amp;amp;_cdi=5231&amp;_sort=d&amp;amp;amp;amp;amp;amp;amp;amp;view=c&amp;_acct=C000006878&amp;amp;_version=1&amp;_urlVersion=0&amp;amp;_userid=4140103&amp;md5=646ce5a276#cor1"&gt;&lt;/a&gt;, &lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;amp;amp;amp;amp;amp;amp;amp;_udi=B6TFN-4KX00R3-5&amp;_coverDate=09%2F16%2F2006&amp;amp;_alid=456445778&amp;_rdoc=1&amp;amp;_fmt=&amp;_orig=search&amp;amp;amp;amp;amp;amp;amp;amp;_qd=1&amp;_cdi=5231&amp;amp;_sort=d&amp;view=c&amp;amp;_acct=C000006878&amp;_version=1&amp;amp;_urlVersion=0&amp;_userid=4140103&amp;amp;md5=646ce5a276#implicit0"&gt;a&lt;/a&gt;, &lt;a href="mailto:wilson.barros@vanderbilt.edu"&gt;&lt;/a&gt;and Daniel F. Gochberg&lt;br /&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6TFN-4KX00R3-5&amp;amp;amp;amp;amp;amp;amp;amp;_coverDate=09%2F16%2F2006&amp;_alid=456445778&amp;amp;_rdoc=1&amp;_fmt=&amp;amp;_orig=search&amp;_qd=1&amp;amp;_cdi=5231&amp;_sort=d&amp;amp;amp;amp;amp;amp;amp;amp;view=c&amp;_acct=C000006878&amp;amp;_version=1&amp;_urlVersion=0&amp;amp;_userid=4140103&amp;amp;md5=646ce5a276#implicit0"&gt;a&lt;/a&gt; &lt;a name="implicit0"&gt;&lt;/a&gt;aVanderbilt University Institute of Imaging Science (VUIIS), Vanderbilt University Medical Center, R-1302 Medical Center North, Nashville, TN 37232-2310&lt;br /&gt;&lt;br /&gt;Here we show that simultaneous measurement of the self-diffusioncoefficient D and the relaxation time T2 using the NMR signal in the presence of long-range dipolar interactions can be performed using a single-square gradient pulse. Furthermore, during acquisition, a train of 180 radio-frequency pulses is utilized in order to improve signal-to-noise efficiency and to reduce the diffusion-attenuation associated with local field inhomogeneities. The new approach can determine D and T2 in a single-shot acquisition. The results obtained for water protons show good agreement when compared to standard techniques. Finally, this method offers a new possibility for monitoring fast processes.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-115930864969935012?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2006.09.033' title='Fast single-gradient simultaneous measurement of D and T2 in liquids via the distant dipolar field'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/115930864969935012/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=115930864969935012&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115930864969935012'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115930864969935012'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/09/fast-single-gradient-simultaneous.html' title='Fast single-gradient simultaneous measurement of D and T2 in liquids via the distant dipolar field'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-115930828504130655</id><published>2006-09-26T16:59:00.000-05:00</published><updated>2006-09-26T17:04:45.086-05:00</updated><title type='text'>Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications</title><content type='html'>David Z. Balla, Gerd Melkus, Cornelius Faber *&lt;br /&gt;Department of Experimental Physics 5, University of Würzburg, Würzburg, Germany&lt;br /&gt;email: Cornelius Faber (&lt;a href="mailto:faber@physik.uni-wuerzburg.de"&gt;faber@physik.uni-wuerzburg.de&lt;/a&gt;)&lt;br /&gt;*Correspondence to Cornelius Faber, Experimentelle Physik 5, Universität Würzburg, Am Hubland, 97074 Würzburg, Germany&lt;br /&gt;setDOI("ADOI=10.1002/mrm.21007")&lt;br /&gt;Funded by: Deutsche Forschungsgemeinschaft; Grant Number: Fa474/1, Ha1232/13&lt;br /&gt;&lt;a name="keywords"&gt;Keywords&lt;/a&gt;&lt;br /&gt;iZQC • HOMOGENIZED • localized spectroscopy • inhomogeneous broadening • resolution enhancement&lt;br /&gt;&lt;a name="abstract"&gt;Abstract&lt;/a&gt;&lt;br /&gt;Magnetic resonance spectroscopy (MRS) techniques that use the distant dipolar field (DDF) to locally refocus inhomogeneous line-broadening promise improved spectral resolution in spatially varying fields. We investigated three possible implementations of localized DDF spectroscopy. Theoretical analysis and phantom experiments at 17.6 T showed that only localization immediately prior to acquisition provides sufficient spatial selectivity and sensitivity for in vivo applications. Spectra from an (8 mm)3 voxel of the rat brain were acquired in 25 min, and three major metabolites were resolved. In a tumor mouse model, DDF spectra with well-resolved lines can be obtained from significantly larger voxels compared to conventional localized spectroscopy. From an inhomogeneous voxel, improved spectral resolution can be obtained with DDF techniques when a sufficient number of increments are sampled along the second spectral dimension. With fewer increments, measurement time is significantly shortened, and DDF techniques can provide higher signal-to-noise ratio (SNR) efficiency. Magn Reson Med, 2006. © 2006 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-115930828504130655?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21007' title='Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/115930828504130655/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=115930828504130655&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115930828504130655'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115930828504130655'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/09/spatially-localized-intermolecular.html' title='Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-115756668181389938</id><published>2006-09-06T13:10:00.000-05:00</published><updated>2006-09-06T15:18:43.693-05:00</updated><title type='text'>iDQC MRI weighted by longitudinal relaxation in the rotating frame</title><content type='html'>Bingwen Zheng, Zhong Chen, Scott D. Kennedy, and Jianhui Zhong&lt;br /&gt;&lt;a name="abstract"&gt;&lt;/a&gt;&lt;br /&gt;A long-duration, low-power, off-resonance spin-locking pulse was incorporated into the COSY revamped by asymmetric z gradient-echo detection (CRAZED) pulse sequence in order to evaluate the effects of intermolecular double-quantum longitudinal relaxation in the tilted rotating frame (T[stack 1,DQeff ]). This modified CRAZED sequence was followed by a standard fast spin-echo imaging sequence to form images with T[stack 1,DQeff ]-weighted contrast. Imaging experiments were performed on an agarose-gel phantom and mouse-tail tissue at 600 MHz. Experimental results demonstrated the feasibility of imaging applications based on T[stack 1,DQeff ] as a novel contrast mechanism, and showed that iDQC off-resonance longitudinal relaxation in the rotating frame T[stack 1,DQeff ] is sensitive to the tilt angle and the effective spin-locking field e. Imaging based on T[stack 1,DQeff ] has reduced RF power deposition compared to on-resonance spin-locking, which is advantageous for human applications. Magn Reson Med, 2006. © 2006 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-115756668181389938?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.20954' title='iDQC MRI weighted by longitudinal relaxation in the rotating frame'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/115756668181389938/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=115756668181389938&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115756668181389938'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115756668181389938'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/09/idqc-mri-weighted-by-longitudinal.html' title='iDQC MRI weighted by longitudinal relaxation in the rotating frame'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-115645452221103887</id><published>2006-08-24T16:19:00.000-05:00</published><updated>2006-08-24T16:22:02.223-05:00</updated><title type='text'>Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications</title><content type='html'>&lt;h2&gt;&lt;a href="http://www3.interscience.wiley.com/cgi-bin/jhome/10005196"&gt;&lt;/a&gt;&lt;/h2&gt; Magnetic Resonance in Medicine&lt;br /&gt;Early View          (Articles online in advance of print)&lt;br /&gt;David Z. Balla, Gerd Melkus, Cornelius Faber&lt;br /&gt;&lt;br /&gt;Magnetic resonance spectroscopy (MRS) techniques that use the distant dipolar field (DDF) to locally refocus inhomogeneous line-broadening promise improved spectral resolution in spatially varying fields. We investigated three possible implementations of localized DDF spectroscopy. Theoretical analysis and phantom experiments at 17.6 T showed that only localization immediately prior to acquisition provides sufficient spatial selectivity and sensitivity for in vivo applications. Spectra from an (8 mm)&lt;sup&gt;3&lt;/sup&gt; voxel of the rat brain were acquired in 25 min, and three major metabolites were resolved. In a tumor mouse model, DDF spectra with well-resolved lines can be obtained from significantly larger voxels compared to conventional localized spectroscopy. From an inhomogeneous voxel, improved spectral resolution can be obtained with DDF techniques when a sufficient number of increments are sampled along the second spectral dimension. With fewer increments, measurement time is significantly shortened, and DDF techniques can provide higher signal-to-noise ratio (SNR) efficiency. Magn Reson Med, 2006. © 2006 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-115645452221103887?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.21007' title='Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/115645452221103887/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=115645452221103887&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115645452221103887'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/115645452221103887'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/08/spatially-localized-intermolecular.html' title='Spatially localized intermolecular zero-quantum coherence spectroscopy for in vivo applications'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114839558069078231</id><published>2006-05-23T09:43:00.001-05:00</published><updated>2006-05-23T09:46:20.703-05:00</updated><title type='text'>Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI</title><content type='html'>doi is not active yet, for now try this...&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114839558069078231?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www.sciencedirect.com/science/article/B6WJX-4K12CHR-2/2/50ce9e27703c0ca2c05480127e46b8ba' title='Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114839558069078231/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114839558069078231&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114839558069078231'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114839558069078231'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/05/sensitivity-to-local-dipol_114839558069078231.html' title='Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114839442257765421</id><published>2006-05-23T09:25:00.000-05:00</published><updated>2006-05-23T09:27:02.603-05:00</updated><title type='text'>Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI</title><content type='html'>&lt;strong&gt;&lt;/strong&gt;Cornelius Faber,  Carolin Heil, Benjamin Zahneisen, David Z. Balla and Richard Bowtell&lt;br /&gt;                  Journal of Magnetic Resonance                                       &lt;br /&gt;Article in Press,         Corrected Proof&lt;span style="font-size: smaller; font-family: Verdana;"&gt;&lt;span style="color:#ff0000;"&gt;&lt;br /&gt;&lt;/span&gt; &lt;/span&gt;&lt;br /&gt;Local dipole fields such as those created by small iron-oxide particles are used to produce regions of low intensity (dark contrast) in many molecular magnetic resonance imaging applications. We have investigated, with computer simulations and experiments at 17.6 T, how the COSY revamped with asymmetric &lt;i&gt;z&lt;/i&gt;-gradient echo detection (CRAZED) experiment that selects intermolecular double-quantum coherences can also be used to visualize such local dipole fields. Application of the coherence-selection gradient pulses parallel to the main magnetic field produced similar, dark contrast as conventional gradient echo imaging. Application of the gradient along the magic angle leads to total loss of signal intensity in homogeneous samples. In the presence of local dipole fields, the contrast was inverted and bright signals from the dipoles were observed over a very low background. Both simulations and experiments showed that the signal strongly decreased when a phase-cycle suppressing single-quantum coherences was employed. Therefore, we conclude that most of the signal comes from directly refocused magnetization or intermolecular single-quantum coherences. Finally, we demonstrate that bright contrast from local dipole fields can also be obtained, when the pair of coherence-selection gradient pulses is deliberately mismatched. Both methods allowed visualization of local dipole fields in phantoms in experimental times of about 3 min.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114839442257765421?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2006.05.002' title='Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114839442257765421/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114839442257765421&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114839442257765421'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114839442257765421'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/05/sensitivity-to-local-dipole-fields-in.html' title='Sensitivity to local dipole fields in the CRAZED experiment: An approach to bright spot MRI'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114752957998987357</id><published>2006-05-13T09:10:00.000-05:00</published><updated>2007-05-01T09:56:31.572-05:00</updated><title type='text'>Indirect detection of nuclear magnetic resonance via geometrically induced long-range dipolar fields</title><content type='html'>by &lt;strong&gt;C.A. Meriles&lt;a name="bcor1"&gt;&lt;/a&gt; and Wei Dong &lt;/strong&gt;&lt;br /&gt;Department of Physics, CUNY—City College of New York, 138th Street and Convent Avenue, New&lt;br /&gt;York, NY 10031, USA&lt;br /&gt;&lt;p&gt;In press on the Journal of Magnetic Resonance&lt;br /&gt; &lt;/p&gt; &lt;p&gt;We report the indirect detection of the magnetization of one spin species via the NMR signal of a second species. Our method relies on the control of long-range dipolar fields between two separate objects, in this case, a water droplet (sensor) immersed in a tube containing mineral oil (sample). Unlike prior experiments, no gradient pulses are used; rather, the setup geometry is exploited to select the part of the sample to be probed and modulate the spin alignment in the sensor. Our results are discussed in the context of Dipolar Field Microscopy, a proposed strategy in which the detector is a hyperpolarized tip. &lt;/p&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114752957998987357?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2007.02.012' title='Indirect detection of nuclear magnetic resonance via geometrically induced long-range dipolar fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114752957998987357/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114752957998987357&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114752957998987357'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114752957998987357'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/05/indirect-detection-of-nuclear-magnetic.html' title='Indirect detection of nuclear magnetic resonance via geometrically induced long-range dipolar fields'/><author><name>Mauro A.</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114605914129972318</id><published>2006-04-26T08:37:00.000-05:00</published><updated>2006-04-26T08:45:41.310-05:00</updated><title type='text'>A new approach to bright spot MRI: visualizing local dipolar fields with the CRAZED sequence</title><content type='html'>At ISMRM...&lt;br /&gt;&lt;br /&gt;2478. A new approach to bright spot MRI: visualizing local dipolar fields with the CRAZED sequence&lt;br /&gt;&lt;br /&gt;Cornelius Faber, Carolin Heil, Benjamin Zahneisen, David Balla, Richard Bowtell&lt;br /&gt;&lt;br /&gt;EP5, University of Wuerzburg, Germany&lt;br /&gt;SPMMRC, University of Nottingham, UK&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114605914129972318?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://ismrm.org/06/Traditional3b.htm#Contrast_Mechanisms_and_MTC' title='A new approach to bright spot MRI: visualizing local dipolar fields with the CRAZED sequence'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114605914129972318/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114605914129972318&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114605914129972318'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114605914129972318'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/04/new-approach-to-bright-spot-mri.html' title='A new approach to bright spot MRI: visualizing local dipolar fields with the CRAZED sequence'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114555329339108440</id><published>2006-04-20T12:12:00.000-05:00</published><updated>2006-04-20T12:14:53.403-05:00</updated><title type='text'>The transient dynamics leading to spin turbulence in high-field solution magnetic resonance: A numerical study</title><content type='html'>The transient dynamics leading to spin turbulence in high-field solution magnetic resonance: A numerical study&lt;br /&gt;&lt;a href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=ALL&amp;possible1=Datta%2C+Sandip&amp;amp;possible1zone=author&amp;maxdisp=25&amp;amp;smode=strresults&amp;aqs=true"&gt;Sandip Datta&lt;/a&gt;, &lt;a href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=ALL&amp;amp;possible1=Huang%2C+Susie+Y.&amp;possible1zone=author&amp;amp;maxdisp=25&amp;smode=strresults&amp;amp;aqs=true"&gt;Susie Y. Huang&lt;/a&gt;, and &lt;a href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=ALL&amp;possible1=Lin%2C+Yung-Ya&amp;amp;possible1zone=author&amp;maxdisp=25&amp;amp;smode=strresults&amp;aqs=true"&gt;Yung-Ya Lin&lt;/a&gt;&lt;br /&gt;Department of Chemistry and Biochemistry, University of California, Los Angeles, California 90095&lt;br /&gt;(Received 16 September 2005; accepted 7 February 2006; published online 17 April 2006)&lt;br /&gt;The dynamics under the joint action of radiation damping and the distant dipolar field in high-field solution magnetic resonance are investigated. Different dynamical regimes during the evolution are identified and their individual features are discussed. In the steady state, the dynamics can be associated with a strange attractor in phase space on which the motion is chaotic. The possibility of the observed chaotic motion being spatiotemporal is examined. ©2006 American Institute of Physics&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114555329339108440?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114555329339108440/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114555329339108440&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114555329339108440'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114555329339108440'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/04/transient-dynamics-leading-to-spin.html' title='The transient dynamics leading to spin turbulence in high-field solution magnetic resonance: A numerical study'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114521846467587761</id><published>2006-04-16T13:50:00.000-05:00</published><updated>2006-04-16T15:14:24.706-05:00</updated><title type='text'>DDF/iZQC at ISMRM in Seattle</title><content type='html'>Please post if I missed one...Thanks, Curt&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;Room 4E                    Monday 14:00 -   16:00&lt;br /&gt;&lt;b&gt;&lt;i&gt;1032&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;Simulations of Motion-Insensitive Diffusion Imaging Based on the  Distant Dipolar Field&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt; &lt;p class="ISMRMAuthors"&gt;Tao Lin&lt;sup&gt;1&lt;/sup&gt;, Huijun Sun&lt;sup&gt;1&lt;/sup&gt;, Congbo Cai&lt;sup&gt;1&lt;/sup&gt;,  Zhong Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;, Shuhui Cai&lt;sup&gt;1&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;br /&gt;&lt;a name="Clinical_MRS_in_Cancer"&gt;&lt;br /&gt;&lt;/a&gt; &lt;div  style="border-style: none none solid; padding: 0pt 0pt 1pt;color:-moz-use-text-color -moz-use-text-color windowtext;"&gt;  &lt;p class="ISMRMSessionSubHead"&gt;&lt;br /&gt;Room 4E                    Tuesday 13:30 -   15:30&lt;i&gt;&lt;span style="font-weight: bold;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/i&gt;&lt;/p&gt;&lt;p class="ISMRMSessionSubHead"&gt;&lt;i&gt;&lt;span style="font-weight: bold;"&gt;&lt;/span&gt;2423&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;MR Imaging of Intermolecular Double-Quantum-Filtered Zero-Quantum  Coherence&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt;&lt;/div&gt;&lt;b&gt;&lt;/b&gt; &lt;p class="ISMRMAuthors"&gt;Zhong Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;, Bingwen Zheng&lt;sup&gt;1&lt;/sup&gt;,  Xiaoqin Zhu&lt;sup&gt;1&lt;/sup&gt;, Tianliang Gu&lt;sup&gt;2&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;br /&gt;&lt;br /&gt;Room 4E                    Wednesday 14:00 -   16:00&lt;br /&gt;&lt;b&gt;&lt;i&gt;2479&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;Effect of Distant Dipolar Field and &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt; on  Magnetization in CRAZED-Multiecho Pulse Sequence&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt;  &lt;p class="ISMRMAuthors"&gt;Chung Ki Wong&lt;sup&gt;1&lt;/sup&gt;, Edmund Kwok&lt;sup&gt;1&lt;/sup&gt;,  Jianhui Zhong&lt;sup&gt;1&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt;  &lt;sup&gt;1&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;br /&gt;&lt;br /&gt;Room 4E                    Thursday 13:30 -   15:30&lt;br /&gt;&lt;b&gt;&lt;i&gt;3020&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;Spectroscopic and Imaging Observations of Intermolecular  Single-Quantum Coherence&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt; &lt;p class="ISMRMAuthors"&gt;Shuhui Cai&lt;sup&gt;1&lt;/sup&gt;, Zhong Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;,  Xiaoqin Zhu&lt;sup&gt;1&lt;/sup&gt;, Bingwen Zheng&lt;sup&gt;1&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;br /&gt;&lt;br /&gt;&lt;b&gt;&lt;i&gt;3040&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;Intermolecular Double-Quantum-Filtered Zero-Quantum Coherence in  Liquid NMR&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt; &lt;p class="ISMRMAuthors"&gt;Xiaoqin Zhu&lt;sup&gt;1&lt;/sup&gt;, Zhong Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;,  Shuhui Cai&lt;sup&gt;1&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;br /&gt;&lt;br /&gt;&lt;b&gt;&lt;i&gt;3046&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;POM: A Simulation Program for NMR Under Inter- And Intramolecular  Interactions&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt; &lt;p class="ISMRMAuthors"&gt;Congbo Cai&lt;sup&gt;1&lt;/sup&gt;, Zhong Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;,  Shuhui Cai&lt;sup&gt;1&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;p class="ISMRMAffiliations"&gt;&lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;p class="ISMRMProgramEntry"&gt;&lt;!--[if gte vml 1]&gt;&lt;v:shape id="_x0000_s1131" type="#_x0000_t202" style="'position:absolute;margin-left:0;margin-top:10.5pt;" filled="f" stroked="f"&gt;  &lt;v:textbox inset="0,0,0,0"&gt; &lt;p class="MsoNormal"&gt;&lt;span style="font-size: 9.0pt; mso-bidi-font-size: 12.0pt"&gt; &lt;o:p&gt; &lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;  &lt;/v:textbox&gt; &lt;/v:shape&gt;&lt;![endif]--&gt;&lt;!--[if !vml]--&gt;&lt;span style="position: absolute; z-index: 417; left: 43px; top: 14521px; width: 1px; height: 19px;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;!--[endif]--&gt;&lt;/p&gt; &lt;!--[if !mso]--&gt;&lt;!--[endif]--&gt;&lt;p&gt;&lt;b&gt;&lt;i&gt;3047&lt;span class="ISMRMProgramNumber"&gt;.    &lt;/span&gt;&lt;/i&gt;Simultaneous Acquisition of Signals of Different Orders of  Intermolecular&lt;br /&gt;                                 Multiple-Quantum Coherences&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/b&gt;&lt;/p&gt; &lt;p class="ISMRMAuthors"&gt;Song Chen&lt;sup&gt;1&lt;/sup&gt;, Xiaoqin Zhu&lt;sup&gt;1&lt;/sup&gt;, Zhong  Chen&lt;sup&gt;1&lt;/sup&gt;,&lt;sup&gt; 2&lt;/sup&gt;, Shuhui Cai&lt;sup&gt;1&lt;/sup&gt;, Jianhui Zhong&lt;sup&gt;2&lt;/sup&gt;&lt;span class="ISMRMTitle"&gt;&lt;/span&gt;&lt;/p&gt; &lt;sup&gt;1&lt;/sup&gt;Xiamen University, Xiamen, Fujian,  People’s Republic of China; &lt;sup&gt;2&lt;/sup&gt;University of Rochester, Rochester, New  York, USA&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114521846467587761?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://ismrm.org/06/' title='DDF/iZQC at ISMRM in Seattle'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114521846467587761/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114521846467587761&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114521846467587761'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114521846467587761'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/04/ddfizqc-at-ismrm-in-seattle.html' title='DDF/iZQC at ISMRM in Seattle'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114517602753087800</id><published>2006-04-16T03:21:00.000-05:00</published><updated>2006-04-16T03:27:07.546-05:00</updated><title type='text'>ENC next week</title><content type='html'>Spin Locking SQCs in an iMQC Experiment&lt;br /&gt;&lt;br /&gt;                                          Gigi Galiana1; Rosa T. Branca2; Warren S. Warren2;&lt;br /&gt;                               1Princeton University, Princeton, NJ; 2Duke University, Durham, NC;&lt;br /&gt;&lt;br /&gt;While iMQCs present a wide range of promising applications, dephasing during t2 competes with signal buildup, and limits the maximum attainable signal. Previous work has explored signal with T1ρ decay during t1, where iMQC terms like IxSx can be locked with a steady RF field along x. In reality, many Cartesian terms that do not lie along the locking axis can also be conserved with a spinlocking pulse. For example, antiphase terms such as IxSz–IzSx, are perfectly locked with a spinlock along y, and continue to be locked when they evolve into observable magnetization. Based on this principle, we present a method to slow the effective dephasing rate during the signal build up period to enhance the iMQC signal.&lt;br /&gt;&lt;br /&gt;                      Distant Dipolar Field Effects in Polymer Melts: A new Approach  &lt;br /&gt;                                 Towards  Structural Investigations Of Complex Fluids&lt;br /&gt;&lt;br /&gt;                                                    Priyanga Bandara; Marcel Utz;&lt;br /&gt;                                        University of Connecticut, Storrs, CT, United States&lt;br /&gt;&lt;br /&gt;We report the observation of distant dipolar field (DDF) effects in polymer melts. Using the CRAZED sequence, we have succeeded in obtaining DDF double quantum echos in melts of poly(isobutylene). In this system, T2is about 2ms. This requires the use of very strong gradient pulses, which are generated using a home-built gradient probe assembly with a car battery as current source. Experiments of this type could be very useful to investigate the structure of polymer systems. Motivated by such applications, we report pilot measurements using a suspension of PTFE spheres of various diameters in PIB.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;            Intermolecular Zero Quantum Spectroscopy in the Live Mouse Brain Using a MR Imager&lt;br /&gt;                                        Benoit M. Boulat; P.T. Narasimhan; Russell E. Jacobs;&lt;br /&gt;                                                                    Caltech, Pasadena, CA&lt;br /&gt;&lt;br /&gt;We have utilized the effects of the distant dipolar field to obtain one-dimensional high-resolution NMR spectra in the full head or a localized region in the brain of live mice. Experiments were conducted on a 11.7T magnetic resonance imager. The method uses techniques of two-dimensional NMR spectroscopy and can be well described within the formalism known as “Intermolecular Zero Quantum (IZQ) spectroscopy”. Based on HOMOGENIZED class of pulse sequences, IZQ spectra of good resolution and signal to noise ratio could be obtained in as little as 18 minutes. The method was utilized to study mice of various genetic background.&lt;br /&gt;&lt;br /&gt;         In vivo multiple quantum imaging of prostatic ductal structure by MR: preliminary results&lt;br /&gt;&lt;br /&gt;                Albert P Chen1; Charles H Cunningham2; Louis-S Bouchard3; Janine Lupo1; John M  &lt;br /&gt;                 Pauly2; Danial B Vigneron1;&lt;br /&gt;&lt;br /&gt;1University of California, San Francisco, San Francisco, CA; 2Stanford University, Stanford, CA; 3University of California, Berkeley and LBNL, Berkeley, CA;&lt;br /&gt;&lt;br /&gt;The glandular prostate consists of a duct system that can not be resolved by conventional MRI at lower or moderate field strength (1.5T-3T). Intermolecular multiple quantum coherence (iMQC) that arises from long-range nuclear dipole-dipole couplings has been shown to have the ability to encode spatial heterogeneity on an intermediate length scale using a CRAZED sequence. With this method, structural anisotropy of a given material not detected by MR diffusion methods have been observed in heterogeneous media. This preliminary study demonstrates for the first time the feasibility of obtaining CRAZED images from the prostate in vivo. Potentially, CRAZED may provide a unique image contrast based on the ductal structural anisotropy.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;                               Fast simultaneous measurement of D and T2 using the distant dipolar field&lt;br /&gt;                                   &lt;br /&gt;                                                          Wilson Barros Jr; Daniel F. Gochberg;&lt;br /&gt;                                    Vanderbilt University Institute of Imaging Science, Nashville, TN&lt;br /&gt;&lt;br /&gt;Recently, we reported the simultaneous measurement of the self-diffusion coefficient D and the&lt;br /&gt;spin-spin relaxation time T2 via the NMR signal refocused by long-range dipolar field interactions. Typically the signal available for this methodology is a fraction of the full equilibrium magnetization density. Here, we incorporated a train of equally spaced π pulses into the standard CRAZED (COSY Revamped by Asymmetric Z-gradient Echo Detection) sequence in order to improve the signal-to-noise ratio as well as to perform fast acquisition. A reduction of undesirable diffusion-attenuation caused by local magnetic-field inhomogeneities is also realized. In a series of experiments, the parameters D and T2 are extracted by this method and then compared to values obtained by conventional techniques.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114517602753087800?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114517602753087800/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114517602753087800&amp;isPopup=true' title='2 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114517602753087800'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114517602753087800'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/04/enc-next-week.html' title='ENC next week'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>2</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-114365322760908244</id><published>2006-03-29T11:23:00.000-06:00</published><updated>2006-03-29T11:31:30.116-06:00</updated><title type='text'>iMQC Discussion at ISMRM</title><content type='html'>I'd like to propose a discussion group, get together at ISMRM in Seattle.&lt;br /&gt;&lt;br /&gt;Maybe a dinner or lunch as well if folks are interested?&lt;br /&gt;&lt;br /&gt;What do you think?&lt;br /&gt;&lt;br /&gt;-Curt&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-114365322760908244?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='mailto:corum@cmrr.umn.edu' title='iMQC Discussion at ISMRM'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/114365322760908244/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=114365322760908244&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114365322760908244'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/114365322760908244'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/03/imqc-discussion-at-ismrm.html' title='iMQC Discussion at ISMRM'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-113986627710538782</id><published>2006-02-13T15:29:00.000-06:00</published><updated>2006-02-17T10:54:53.290-06:00</updated><title type='text'>Formation and identification of pure intermolecular zero-quantum coherence signal in liquid NMR</title><content type='html'>Xiaoqin Zhu, Zhong Chen, Shuhui Cai and Jianhui Zhong&lt;br /&gt;&lt;br /&gt;A new pulse sequence with three radio-frequency pulses was designed to detect NMR signals originating from pure intermolecular zero-quantum coherence (iZQC) in isolated spin-1/2 samples such as water. Analytical expressions were derived from the modified Bloch equations with dipolar fields. All the experimental observations and simulated results demonstrate that the iZQC signals can be selectively detected, mostly free of contamination of other coherences and conventional signals. Compared to the two-pulse CRAZED sequence, the new sequence is insensitive to the imperfection of flip angles.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-113986627710538782?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2006.01.041' title='Formation and identification of pure intermolecular zero-quantum coherence signal in liquid NMR'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/113986627710538782/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=113986627710538782&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113986627710538782'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113986627710538782'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/02/formation-and-identification-of-pure.html' title='Formation and identification of pure intermolecular zero-quantum coherence signal in liquid NMR'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03004469704141377241</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-113926543855298523</id><published>2006-02-06T16:36:00.000-06:00</published><updated>2006-02-06T16:38:25.433-06:00</updated><title type='text'>International Symposium on Biomedical Magnetic Resonance Imaging and Spectroscopy at Very High Fields</title><content type='html'>University of Wuerzburg&lt;br /&gt;Institute of Physics&lt;br /&gt;Am Hubland&lt;br /&gt;97074 Wuerzburg&lt;br /&gt;Germany&lt;br /&gt;2/16-2/18&lt;br /&gt;Two sessions on IMQC&lt;br /&gt;Intermolecular Multiple-quantum Coherences&lt;br /&gt;Intermolecular Multiple-quantum Coherences II&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-113926543855298523?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://bio.physik.uni-wuerzburg.de/hf/' title='International Symposium on Biomedical Magnetic Resonance Imaging and Spectroscopy at Very High Fields'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/113926543855298523/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=113926543855298523&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113926543855298523'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113926543855298523'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2006/02/international-symposium-on-biomedical.html' title='International Symposium on Biomedical Magnetic Resonance Imaging and Spectroscopy at Very High Fields'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-113292187362702071</id><published>2005-11-25T06:22:00.000-06:00</published><updated>2005-11-25T06:31:13.636-06:00</updated><title type='text'>Ultrafast Intermolecular Zero Quantum Spectroscopy</title><content type='html'>&lt;p&gt;  &lt;au&gt;Gigi Galiana,&lt;/au&gt;  &lt;au&gt;Rosa T. Branca, and&lt;/au&gt;  &lt;au&gt;Warren S. Warren&lt;/au&gt;  &lt;/p&gt; &lt;aff&gt;&lt;/aff&gt;&lt;ti&gt;J. Am. Chem. Soc., in press (2005)&lt;/ti&gt;&lt;br /&gt;&lt;br /&gt;Clinical magnetic resonance spectroscopy is typically limited by magnetic inhomogeneities which destroy spectral resolution, but intermolecular zero quantum coherences (iZQCs) are insensitive to such inhomogeneities. iZQC resolution in vivo, however, has been hampered by physiological fluctuations over the time scale of the two-dimensional acquisition. A faster iZQC sequence will allow us to average away these fluctuations, and thus we present a new approach to ultrafast two-dimensional spectroscopy. This communication reports iZQC experiments acquiring up to 31 t1-points per scan, as well as extensions to a broad range of other 2D sequences.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-113292187362702071?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1021/ja054463m' title='Ultrafast Intermolecular Zero Quantum Spectroscopy'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/113292187362702071/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=113292187362702071&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113292187362702071'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113292187362702071'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/11/ultrafast-intermolecular-zero-quantum.html' title='Ultrafast Intermolecular Zero Quantum Spectroscopy'/><author><name>Mauro A.</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-113198710218866885</id><published>2005-11-14T10:49:00.000-06:00</published><updated>2005-11-14T10:51:42.200-06:00</updated><title type='text'>Intermolecular multiple quantum coherences at high magnetic field: The nonlinear regime</title><content type='html'>&lt;a style="font-family: times new roman;" href="http://scitation.aip.org/vsearch/servlet/VerityServlet?KEY=ALL&amp;possible1=Marques%2C+J.+P.&amp;amp;possible1zone=author&amp;maxdisp=25&amp;amp;smode=strresults&amp;aqs=true"&gt;&lt;/a&gt;J. P. Marques, S. Grant, S. Blackband, R. W. Bowtell&lt;br /&gt;J. Chem. Phys. &lt;b&gt;123&lt;/b&gt;, 164311 (2005) &lt;i&gt;(10 pages)&lt;br /&gt;&lt;br /&gt;&lt;/i&gt;  Experiments&lt;sup&gt; &lt;/sup&gt;have been carried at magnetic-field strengths of 9.4, 14.1, and&lt;sup&gt; &lt;/sup&gt;17.6 T to explore the evolution of intermolecular multiple quantum&lt;sup&gt; &lt;/sup&gt;coherences in the nonlinear regime where the system evolves for&lt;sup&gt; &lt;/sup&gt;times that are much greater than the characteristic time of&lt;sup&gt; &lt;/sup&gt;action of the long-range dipolar field, &lt;img src="http://scitation.aip.org/stockgif3/tgr.gif" alt="tau" align="bottom" border="0" /&gt;&lt;sub&gt;&lt;i&gt;d&lt;/i&gt;&lt;/sub&gt;. The results show&lt;sup&gt; &lt;/sup&gt;the expected Bessel function form of the recorded signal as&lt;sup&gt; &lt;/sup&gt;a function of time of evolution, with evident zeros and&lt;sup&gt; &lt;/sup&gt;sign changes. As expected, the rate of signal evolution increases&lt;sup&gt; &lt;/sup&gt;at higher-field strengths as a result of the increased equilibrium&lt;sup&gt; &lt;/sup&gt;magnetization. A numerical method for calculating the evolution of magnetization&lt;sup&gt; &lt;/sup&gt;under the action of the distant dipolar field, relaxation, and&lt;sup&gt; &lt;/sup&gt;diffusion that is based on Fourier analysis of the magnetization&lt;sup&gt; &lt;/sup&gt;distribution has been applied to the correlated two-dimensional spectroscopy revamped&lt;sup&gt; &lt;/sup&gt;by asymmetric &lt;i&gt;z&lt;/i&gt;-gradient echo detection sequence in the nonlinear regime&lt;sup&gt; &lt;/sup&gt;and shown to produce results that are in good agreement&lt;sup&gt; &lt;/sup&gt;with experimental data acquired at different magnetic fields and rates&lt;sup&gt; &lt;/sup&gt;of spatial modulation. Experiments and simulations have also been used&lt;sup&gt; &lt;/sup&gt;to explore the evolution of magnetization in a mixture of&lt;sup&gt; &lt;/sup&gt;two interacting spin species in the nonlinear regime.      ©2005 &lt;i&gt;American Institute of Physics&lt;/i&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-113198710218866885?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1063/1.2085169' title='Intermolecular multiple quantum coherences at high magnetic field: The nonlinear regime'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/113198710218866885/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=113198710218866885&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113198710218866885'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113198710218866885'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/11/intermolecular-multiple-quantum.html' title='Intermolecular multiple quantum coherences at high magnetic field: The nonlinear regime'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-113155763652272170</id><published>2005-11-09T11:31:00.000-06:00</published><updated>2005-11-14T10:59:49.120-06:00</updated><title type='text'>Simultaneous measurement of D and T2 using the distant dipolar field</title><content type='html'>&lt;strong&gt;&lt;/strong&gt;Wilson Barros, Jr., John C. Gore and Daniel F. Gochberg&lt;br /&gt;                   Journal of Magnetic Resonance                                      &lt;br /&gt;Article in Press,         Corrected Proof &lt;span style=";font-family:Verdana;font-size:smaller;"  &gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;The presence of long-range dipolar fields in liquids is known to introduce a non-linear term in the Bloch–Torrey equations which is responsible for many interesting effects in nuclear magnetic resonance as well as in magnetic resonance imaging. We show here, for the first time, that the diffusion coefficient &lt;i&gt;D&lt;/i&gt; and the spin–spin relaxation time &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt; can be obtained simultaneously from the time evolution profile of the long-range dipolar field refocused signal. In a COSY Revamped by Z-asymmetric Echo Detection sequence, the analytical first-order approximation solution of the Bloch–Torrey equations modified to include the effect of the distant dipolar field is used to demonstrate the technique in an experiment using doped water.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-113155763652272170?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.09.013' title='Simultaneous measurement of D and T2 using the distant dipolar field'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/113155763652272170/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=113155763652272170&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113155763652272170'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/113155763652272170'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/11/simultaneous-measurement-of-d-and-t2.html' title='Simultaneous measurement of D and T2 using the distant dipolar field'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112735092314242382</id><published>2005-09-21T19:59:00.000-05:00</published><updated>2005-09-21T20:02:03.153-05:00</updated><title type='text'>Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions</title><content type='html'>Louis-S. Bouchard&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6WJX-4GCX1SH-1&amp;amp;_user=86629&amp;_handle=V-WA-A-W-AZ-MsSAYVA-UUA-U-AAWEDYVCAW-AAWDBZCBAW-BVEECECEZ-AZ-U&amp;amp;_fmt=summary&amp;_coverDate=09%2F30%2F2005&amp;amp;_rdoc=5&amp;_orig=browse&amp;amp;_srch=%23toc%236890%232005%23#aff1"&gt;a&lt;/a&gt;, Felix W. Wehrli&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6WJX-4GCX1SH-1&amp;amp;_user=86629&amp;_handle=V-WA-A-W-AZ-MsSAYVA-UUA-U-AAWEDYVCAW-AAWDBZCBAW-BVEECECEZ-AZ-U&amp;amp;_fmt=summary&amp;_coverDate=09%2F30%2F2005&amp;amp;_rdoc=5&amp;_orig=browse&amp;amp;_srch=%23toc%236890%232005%23#aff2"&gt;b&lt;/a&gt;, Chih-Liang Chin&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6WJX-4GCX1SH-1&amp;amp;_user=86629&amp;_handle=V-WA-A-W-AZ-MsSAYVA-UUA-U-AAWEDYVCAW-AAWDBZCBAW-BVEECECEZ-AZ-U&amp;amp;_fmt=summary&amp;_coverDate=09%2F30%2F2005&amp;amp;_rdoc=5&amp;_orig=browse&amp;amp;_srch=%23toc%236890%232005%23#aff2"&gt;b&lt;/a&gt; and Warren S. Warren&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6WJX-4GCX1SH-1&amp;amp;_user=86629&amp;_handle=V-WA-A-W-AZ-MsSAYVA-UUA-U-AAWEDYVCAW-AAWDBZCBAW-BVEECECEZ-AZ-U&amp;amp;_fmt=summary&amp;_coverDate=09%2F30%2F2005&amp;amp;_rdoc=5&amp;_orig=browse&amp;amp;_srch=%23toc%236890%232005%23#aff1"&gt;a&lt;/a&gt;, &lt;a name="bcor1"&gt;&lt;/a&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=ArticleURL&amp;_udi=B6WJX-4GCX1SH-1&amp;amp;_user=86629&amp;_handle=V-WA-A-W-AZ-MsSAYVA-UUA-U-AAWEDYVCAW-AAWDBZCBAW-BVEECECEZ-AZ-U&amp;amp;_fmt=summary&amp;_coverDate=09%2F30%2F2005&amp;amp;_rdoc=5&amp;_orig=browse&amp;amp;_srch=%23toc%236890%232005%23#cor1"&gt;&lt;/a&gt;, &lt;a href="mailto:wwarren@princeton.edu"&gt;&lt;/a&gt;&lt;a name="aff1"&gt;&lt;/a&gt;aDepartment of Chemistry, Princeton University, Princeton, NJ 08544, USA&lt;a name="aff2"&gt;&lt;/a&gt;bDepartment of Radiology, University of Pennsylvania, Philadelphia, PA 19104, USA Received 19 February 2005;  revised 27 April 2005.  Available online 13 June 2005.&lt;br /&gt;Abstract&lt;br /&gt;We investigate the use of intermolecular multiple-quantum coherence to probe structural anisotropy in trabecular bone. Despite the low volume fraction of bone, the bone–water interface produces internal magnetic field gradients which modulate the dipolar field, depending on sample orientation, choice of dipolar correlation length, correlation gradient direction, and evolution time. For this system, the probing of internal magnetic field gradients in the liquid phase permits indirect measurements of the solid phase dipolar field. Our results suggest that measurements of volume-averaged signal intensity as a function of gradient strength and three orthogonal directions could be used to non-invasively measure the orientation of structures inside a sample or their degree of anisotropy. The system is modeled as having two phases, solid and liquid (bone and water), which differ in their magnetization density and magnetic susceptibility. A simple calculation using a priori knowledge of the material geometry and distribution of internal magnetic fields verifies the experimental measurements as a function of gradient strength, direction, and sample orientation.&lt;br /&gt;Keywords: Distant dipolar field; Intermolecular multiple-quantum coherence; Porous materials; Trabecular bone; Material anisotropy; Microstructure&lt;br /&gt;PACS: 76.60.Jx&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112735092314242382?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.05.012' title='Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112735092314242382/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112735092314242382&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112735092314242382'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112735092314242382'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/09/structural-anisotropy-and-internal.html' title='Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112702807767297221</id><published>2005-09-18T02:16:00.000-05:00</published><updated>2005-09-18T02:24:48.996-05:00</updated><title type='text'>Multiple-quantum vector field imaging by magnetic resonance</title><content type='html'>Louis-S. Bouchard and Warren S. Warren&lt;br /&gt;&lt;br /&gt;Published in J. Magn. Res. 177, 9-21 (2005)&lt;br /&gt;&lt;br /&gt;We introduce a method for non-invasively mapping fiber orientation in materials and biological tissues using intermolecular multiple-quantum coherences. The nuclear magnetic dipole field of water molecules is configured by a CRAZED sequence to encode spatial distributions of material heterogeneities. At any given point &lt;strong&gt;r&lt;/strong&gt; in space, we obtain the spherical coordinates of fiber orientation (&lt;i&gt;θ&lt;/i&gt;,&lt;i&gt;ϕ&lt;/i&gt;) with respect to the external field by comparing three signals &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;, &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;, and &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Z&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; (modulus), acquired with linear gradients applied along the &lt;i&gt;X&lt;/i&gt;, &lt;i&gt;Y&lt;/i&gt;, and &lt;i&gt;Z&lt;/i&gt; axes, respectively. For homogeneous isotropic materials, a subtraction &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Z&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; − &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; − &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; gives zero. With anisotropic materials, we find an empirical relationship relating &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Z&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; − &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; − &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;/(&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; + &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; + &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Z&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;) to the polar angle &lt;i&gt;θ&lt;/i&gt;, while &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; − &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;/(&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;X&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; + &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Y&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt; + &lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;&lt;i&gt;G&lt;/i&gt;&lt;sub&gt;&lt;i&gt;Z&lt;/i&gt;&lt;/sub&gt;&lt;img src="http://www.sciencedirect.com/scidirimg/entities/2225.gif" alt="short parallel" border="0" /&gt;) is related to the azimuthal angle &lt;i&gt;ϕ&lt;/i&gt;. Experiments in structured media confirm the structural sensitivity. This technique can probe length scales not accessible by conventional MRI and diffusion tensor imaging.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112702807767297221?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.06.019' title='Multiple-quantum vector field imaging by magnetic resonance'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112702807767297221/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112702807767297221&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112702807767297221'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112702807767297221'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/09/multiple-quantum-vector-field-imaging.html' title='Multiple-quantum vector field imaging by magnetic resonance'/><author><name>Mauro A.</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112239837941684919</id><published>2005-07-26T12:17:00.000-05:00</published><updated>2005-07-26T12:19:39.423-05:00</updated><title type='text'>Nuclear Magnetic Resonance with the Distant Dipolar Field</title><content type='html'>C. A. Corum&lt;br /&gt;186 pages, 43 figures, Ph.D. Dissertation, University of Arizona,   Optical Sciences Center&lt;br /&gt;&lt;br /&gt;Distant dipolar field (DDF)-based nuclear magnetic resonance is an active research area with many fundamental properties still not well understood. Already several intriguing applications have developed, like HOMOGENIZED and IDEAL spectroscopy, that allow high resolution spectra to be obtained in inhomogeneous fields, such as in-vivo. The theoretical and experimental research in this thesis concentrates on the fundamental signal properties of DDF-based sequences in the presence of relaxation (T1 and T2) and diffusion. A general introduction to magnetic resonance phenomenon is followed by a more in depth introduction to the DDF and its effects. A novel analytical signal equation has been developed to describe the effects of T2 relaxation and diffusing spatially modulated longitudinal spins during the signal build period of an HOMOGENIZED cross peak. Diffusion of the longitudinal spins results in a lengthening of the effective dipolar demagnetization time, delaying the re-phasing of coupled anti-phase states in the quantum picture. In the classical picture the unwinding rate of spatially twisted magnetization is no longer constant, but decays exponentially with time. The expression is experimentally verified for the HOMOGENIZED spectrum of 100mM TSP in H2O at 4.7T. Equations have also been developed for the case of multiple repetition steady state 1d and 2d spectroscopic sequences with incomplete magnetization recovery, leading to spatially varying longitudinal magnetization. Experimental verification has been accomplished by imaging the profile. The equations should be found generally applicable for those interested in DDF-based spectroscopy and imaging.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112239837941684919?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www.arxiv.org/abs/physics/0507103' title='Nuclear Magnetic Resonance with the Distant Dipolar Field'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112239837941684919/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112239837941684919&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239837941684919'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239837941684919'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/nuclear-magnetic-resonance-with.html' title='Nuclear Magnetic Resonance with the Distant Dipolar Field'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112239714858442269</id><published>2005-07-26T11:55:00.000-05:00</published><updated>2005-07-26T11:59:08.586-05:00</updated><title type='text'>Multiple-Quantum Vector Imaging</title><content type='html'>Abstract of talk 420 from ISMRM 2005 Meeting (need password for access)&lt;br /&gt;L-S. Bouchard, W. S. Warren&lt;br /&gt;&lt;br /&gt;A novel methodology based on measurements of the distant dipolar field, or intermolecular multiple-quantum coherences, is presented for tracking the vector orientation of parallel fiber bundles or other anisotropic structures in materials or biological tissues. The method uses a CRAZED sequence (Warren et al., Science 262:2005-9, 1993) with correlation gradient applied along the X, Y and Z axes. A subtraction |Gx|+|Gy|-|Gz| gives a signal when structural anisotropy is present and zero when the material is isotropic. For a material consisting of oriented fibers, the strength of the subtraction is related to the polar angle of the directional vector of the fibers. A comparison of X and Y gradients is related to the azimuthal angle. Experimental results in the petiole of celery show that anisotropy can be readily detected by this method. Tilting the sample with respect to the applied field, and rotating the sample in the transverse plane allow gave subtraction results that are consistent with theoretical calculations and demonstrate its applicability. The method can clearly detect structural anisotropy even for very weak gradient pulses well outside any diffusion-weighted regime. The structure sizes that can be detected are on the order of the length of the correlation distance. Thus, material heterogeneities can be detected on the tens of microns to millimeters scales and the method nicely complements currently existing techniques such as diffusion tensor imaging or high resolution MRI. This method finds potential applications in the materials and biomedical sciences. It could perhaps be of use in detecting tumor vascularity or for mapping trabecular bone anisotropy.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112239714858442269?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://cds.ismrm.org/ismrm-2005/Files/00420.pdf' title='Multiple-Quantum Vector Imaging'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112239714858442269/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112239714858442269&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239714858442269'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239714858442269'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/multiple-quantum-vector-imaging.html' title='Multiple-Quantum Vector Imaging'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112239687136638758</id><published>2005-07-26T11:50:00.000-05:00</published><updated>2005-07-26T11:54:31.373-05:00</updated><title type='text'>Effect of Hypercapnia on the iDQC Response</title><content type='html'>Abstract of talk 117 from ISMRM 2005 Meeting (need password for access)&lt;br /&gt;A. Schäfer, S. Zysset, W. Heinke, H. E. Möller&lt;br /&gt;&lt;br /&gt;To date the origin of the fMRI signal change based on intermolecular double quantum coherences (iDQC) is not well understood. The aim of this work was to investigate the sensitivity to global changes of the cerebral blood flow (CBF) of this method. Global CBF changes can be induced by changing the arterial partial pressure of carbon dioxide due to hypercapnia. While the number of activated voxels was significantly decreased, the percentage signal change was roughly seven-fold increased in iDQC-based imaging as compared to conventional BOLD contrast.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112239687136638758?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://cds.ismrm.org/ismrm-2005/Files/00117.pdf' title='Effect of Hypercapnia on the iDQC Response'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112239687136638758/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112239687136638758&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239687136638758'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112239687136638758'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/effect-of-hypercapnia-on-idqc-response.html' title='Effect of Hypercapnia on the iDQC Response'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112132486682462459</id><published>2005-07-14T02:00:00.000-05:00</published><updated>2005-07-15T17:55:26.073-05:00</updated><title type='text'>Selection of intra- or inter-molecular multiple-quantum coherences in NMR of highly polarized solution</title><content type='html'>Xiaoqin Zhu, Zhong Chen, Shuhui Cai and Jianhui Zhong&lt;br /&gt;published in the Physica B, Condensed matter [0921-4526]  yr:2005 vol:362 iss:1-4&lt;br /&gt;pg: 286 -294&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;Abstract&lt;br /&gt;In highly polarized scalar-coupled liquid systems, nuclear magnetic resonance signals from multiple-quantum coherences (MQCs) may be formed by inter-molecular dipolar and/or intra-molecular scalar couplings. Selection of specific signals can simplify the spectra, which may help us understand the underlying physical mechanisms in complex coupled spin systems. In this paper, a pulse sequence with three selective radio-frequency (RF) pulses and phase cycling was designed for this purpose. For an IpSq (p, &lt;a name="mml5"&gt;&lt;/a&gt;&lt;a title="Click to view the MathML source" style="COLOR: black; TEXT-DECORATION: none" href="http://www.sciencedirect.com/science?_ob=MathURL&amp;_method=retrieve&amp;amp;amp;_udi=B6TVH-4FWKDV8-1&amp;_mathId=mml5&amp;amp;_cdi=5535&amp;_rdoc=1&amp;amp;_ArticleListID=295748489&amp;_acct=C000006878&amp;amp;_version=1&amp;_userid=86629&amp;amp;md5=e63b623a417f6d030cb33d5dc00672f2"&gt;q=1,2,3,…&lt;/a&gt;) spin system, there are three kinds of MQC signals, which originate from intra-molecular I–S, inter-molecular I–S, and inter-molecular S–S (or I–I) coherences. These three kinds of signals can be detected separately by proper phase cycling of RF pulses, which is independent of coupling constants. The intra- and inter-molecular MQC signals can also be detected separately with specific preparation periods, but this method is sensitive to coupling constants. Our theoretical predictions are in good agreement with experimental observations. The method proposed herein can be extended to heteronuclear cases.&lt;br /&gt;Keywords: NMR; Inter-molecular MQCs; Intra-molecular MQCs; Dipolar couplings; Scalar couplings; Phase cycling&lt;br /&gt;PACS: 76.60.−k; 76.80.+y; 75.40.Gb; 39.30.+w&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112132486682462459?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.physb.2005.02.026' title='Selection of intra- or inter-molecular multiple-quantum coherences in NMR of highly polarized solution'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112132486682462459/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112132486682462459&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112132486682462459'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112132486682462459'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/selection-of-intra-or-inter-molecular.html' title='Selection of intra- or inter-molecular multiple-quantum coherences in NMR of highly polarized solution'/><author><name>wilson</name><uri>http://www.blogger.com/profile/03468082153010004518</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112121207810252584</id><published>2005-07-12T18:43:00.000-05:00</published><updated>2005-07-12T18:50:27.990-05:00</updated><title type='text'>Nuclear Magnetic Resonance Studies of Quadrupolar Nuclei and Dipolar Field Effects</title><content type='html'>Jeffry Todd Urban&lt;br /&gt;Ph.D. Dissertation&lt;br /&gt;Doctor of Philosophy in Chemistry&lt;br /&gt;University of California, Berkeley&lt;br /&gt;Advisor: Professor Alexander Pines&lt;br /&gt;2004&lt;br /&gt;&lt;br /&gt;Experimental and theoretical research conducted in two areas in the field of nuclear magnetic resonance (NMR) spectroscopy is presented: (1) studies of the coherent quantum-mechanical control of the angular momentum dynamics of quadrupolar (spin I &gt; 1/2) nuclei and its application to the determination of molecular structure; and (2) applications of the long-range nuclear dipolar field to novel NMR detection methodologies. The dissertation is organized into six chapters. The first two chapters and associated appendices are intended to be pedagogical and include an introduction to the quantum-mechanical theory of pulsed NMR spectroscopy and the time dependent theory of quantum mechanics. The third chapter describes investigations of the solid-state multiple-quantum magic angle spinning (MQMAS) NMR experiment applied to I = 5/2 quadrupolar nuclei. This work reports the use of rotary resonance-matched radiofrequency irradiation for sensitivity enhancement of the I = 5/2 MQMAS experiment. These experiments exhibited certain selective line narrowing effects which were investigated theoretically. The fourth chapter extends the discussion of multiple quantum spectroscopy of quadrupolar nuclei to a mostly theoretical study of the feasibility of enhancing the resolution of nitrogen-14 NMR of large biomolecules in solution via double-quantum spectroscopy. The fifth chapter continues to extend the principles of multiple quantum NMR spectroscopy of quadrupolar nuclei to make analogies between experiments in NMR/nuclear quadrupolar resonance (NQR) and experiments in atomic/molecular optics (AMO). These analogies are made through the Hamiltonian and density operator formalism of angular momentum dynamics in the presence of electric and magnetic fields. The sixth chapter investigates the use of the macroscopic nuclear dipolar field to encode the NMR spectrum of an analyte nucleus indirectly in the magnetization of a sensor nucleus. This technique could potentially serve as an encoding module for the recently developed NMR remote detection experiment. The feasibility of using hyperpolarized xenon-129 gas as a sensor is discussed. This work also reports the use of an optical atomic magnetometer to detect the nuclear magnetization of Xe-129 gas, which has potential applicability as a detection module for NMR remote detection experiments.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112121207810252584?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://www-library.lbl.gov/docs/LBNL/567/68/PDF/LBNL-56768.pdf' title='Nuclear Magnetic Resonance Studies of Quadrupolar Nuclei and Dipolar Field Effects'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112121207810252584/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112121207810252584&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112121207810252584'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112121207810252584'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/nuclear-magnetic-resonance-studies-of.html' title='Nuclear Magnetic Resonance Studies of Quadrupolar Nuclei and Dipolar Field Effects'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112120641599072243</id><published>2005-07-12T17:12:00.000-05:00</published><updated>2005-07-12T17:13:35.996-05:00</updated><title type='text'>NMR detection using laser-polarized xenon as a dipolar sensor</title><content type='html'>J. Granwehr, J.T. Urban, A.H. Trabesinger and A. Pines&lt;br /&gt;&lt;span style="font-size: smaller; font-family: Verdana;"&gt;    &lt;a href="http://www.sciencedirect.com/science?_ob=JournalURL&amp;_cdi=6890&amp;amp;_auth=y&amp;_acct=C000032378&amp;amp;_version=1&amp;_urlVersion=0&amp;amp;_userid=616288&amp;md5=441a27172b31716ffc3f0aaa567dfafd"&gt;               &lt;b&gt;&lt;/b&gt;&lt;/a&gt;&lt;/span&gt;Journal of Magnetic Resonance                                       &lt;br /&gt;Article in Press,         Corrected Proof &lt;span style="font-size: smaller; font-family: Verdana;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;Hyperpolarized &lt;sup&gt;129&lt;/sup&gt;Xe can be used as a sensor to indirectly detect NMR spectra of heteronuclei that are neither covalently bound nor necessarily in direct contact with the Xe atoms, but coupled through long-range intermolecular dipole–dipole interactions. To reintroduce long-range dipolar couplings the sample symmetry has to be broken. This can be done either by using an asymmetric sample arrangement, or by breaking the symmetry of the spin magnetization with field gradient pulses. Experiments are performed where only a small fraction of the available &lt;sup&gt;129&lt;/sup&gt;Xe magnetization is used for each point, so that a single batch of xenon suffices for the point-by-point acquisition of a heteronuclear NMR spectrum. Examples with &lt;sup&gt;1&lt;/sup&gt;H as the analyte nucleus show that these methods have the potential to obtain spectra with a resolution that is high enough to determine homonuclear &lt;i&gt;J&lt;/i&gt; couplings. The applicability of this technique with remote detection is discussed.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112120641599072243?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.05.013' title='NMR detection using laser-polarized xenon as a dipolar sensor'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112120641599072243/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112120641599072243&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112120641599072243'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112120641599072243'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/07/nmr-detection-using-laser-polarized.html' title='NMR detection using laser-polarized xenon as a dipolar sensor'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-112013654003343920</id><published>2005-06-30T08:02:00.000-05:00</published><updated>2005-06-30T08:05:33.063-05:00</updated><title type='text'>Solvent-localized NMR spectroscopy using the distant dipolar field: A method for NMR separations with a single gradient</title><content type='html'>Cornelius Faber&lt;br /&gt;Journal of Magnetic Resonance&lt;br /&gt;Article in Press, Corrected Proof&lt;br /&gt;&lt;br /&gt;Solvent-localized NMR (SOLO) is a new method which allows the separation of NMR spectra of substances dissolved in different solvents. It uses the selective HOMOGENIZED pulse sequence to produce a two-dimensional NMR spectrum resulting from intermolecular zero-quantum coherences in one distinct solvent. The detected signal is locally refocused by the action of the distant dipolar field, which is created by a frequency selective pulse only in regions containing the selected solvent. The prerequisites are that the different solvents have sufficiently different chemical shifts to be excited separately and that compartments with different solvents are spatially separated by more than the typical diffusion distance. Here, the method is demonstrated for the solvents water and DMSO on a length scale of 0.5 mm. Because signal in the spectra is refocused locally, SOLO is insensitive to variations in the magnetic field which may result from inhomogeneities or structures in the sample. This makes applications in strongly structured samples possible. SOLO is the first method that achieves localization of NMR signal with a single gradient pulse. Therefore, it can be used in conventional NMR spectrometers with one-axis gradient systems and lends itself to a wide range of applications including in vivo NMR.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-112013654003343920?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.05.014' title='Solvent-localized NMR spectroscopy using the distant dipolar field: A method for NMR separations with a single gradient'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/112013654003343920/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=112013654003343920&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112013654003343920'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/112013654003343920'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/06/solvent-localized-nmr-spectroscopy.html' title='Solvent-localized NMR spectroscopy using the distant dipolar field: A method for NMR separations with a single gradient'/><author><name>Mauro A.</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111944399604462266</id><published>2005-06-22T07:38:00.000-05:00</published><updated>2005-06-22T07:39:56.050-05:00</updated><title type='text'>Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions</title><content type='html'>&lt;strong&gt;&lt;/strong&gt;Louis-S. Bouchard, Felix W. Wehrli, Chih-Liang Chin and Warren S. Warren&lt;br /&gt;Journal of Magnetic Resonance                                       &lt;br /&gt;Article in Press,         Corrected Proof&lt;span style="font-size: smaller; font-family: Verdana;"&gt;&lt;span style="color:#ff0000;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;We investigate the use of intermolecular multiple-quantum coherence to probe structural anisotropy in trabecular bone. Despite the low volume fraction of bone, the bone–water interface produces internal magnetic field gradients which modulate the dipolar field, depending on sample orientation, choice of dipolar correlation length, correlation gradient direction, and evolution time. For this system, the probing of internal magnetic field gradients in the liquid phase permits indirect measurements of the solid phase dipolar field. Our results suggest that measurements of volume-averaged signal intensity as a function of gradient strength and three orthogonal directions could be used to non-invasively measure the orientation of structures inside a sample or their degree of anisotropy. The system is modeled as having two phases, solid and liquid (bone and water), which differ in their magnetization density and magnetic susceptibility. A simple calculation using a priori knowledge of the material geometry and distribution of internal magnetic fields verifies the experimental measurements as a function of gradient strength, direction, and sample orientation.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111944399604462266?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.jmr.2005.05.012' title='Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111944399604462266/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111944399604462266&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111944399604462266'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111944399604462266'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/06/structural-anisotropy-and-internal.html' title='Structural anisotropy and internal magnetic fields in trabecular bone: Coupling solution and solid dipolar interactions'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111886805903826717</id><published>2005-06-15T15:39:00.000-05:00</published><updated>2005-06-15T15:45:00.100-05:00</updated><title type='text'>Finite difference simulation of diffusion behaviors under inter- and intra-molecular multiple-quantum coherences in liquid NMR</title><content type='html'>&lt;strong style="font-weight: normal;"&gt;Congbo Cai, Zhong Chen, Shuhui Cai, Lian-Pin Hwang and Jianhui Zhong&lt;br /&gt;&lt;/strong&gt;&lt;span style=";font-family:Verdana;font-size:smaller;"  &gt;    &lt;a href="http://www.sciencedirect.com/science?_ob=JournalURL&amp;_cdi=5231&amp;amp;amp;_auth=y&amp;_acct=C000032378&amp;amp;_version=1&amp;_urlVersion=0&amp;amp;_userid=616288&amp;md5=8f49c3da53d33109afae123f00ea98cd"&gt;               Chemical Physics Letters      &lt;/a&gt;     &lt;/span&gt;     &lt;span style=";font-family:Verdana;font-size:smaller;"  &gt;                      &lt;br /&gt;&lt;a href="http://www.sciencedirect.com/science?_ob=IssueURL&amp;amp;_tockey=%23TOC%235231%232005%23995929995%23595219%23FLA%23display%23Volume_407,_Issues_4-6,_Pages_243-546_%2827_May_2005%29%23tagged%23Volume%23first%3D407%23Issues%23first%3D4%23last%3D6%23spans%3D3%23date%23%2827_May_2005%29%23&amp;amp;_auth=y&amp;view=c&amp;amp;_acct=C000032378&amp;_version=1&amp;amp;_urlVersion=0&amp;_userid=616288&amp;amp;md5=35da31af5bfe3a55f36876c77d92eaf8"&gt;   Volume 407, Issues 4-6&lt;/a&gt;           ,   27 May 2005,   Pages 438-443&lt;/span&gt;&lt;br /&gt;&lt;strong style="font-weight: normal;"&gt;&lt;br /&gt;&lt;/strong&gt;The behaviors of molecular self-diffusion were simulated in complex spin systems with both intra-molecular scalar couplings and inter-molecular dipolar couplings in liquid nuclear magnetic resonance (NMR). The simulation algorithm was based on a combination of the non-linear Bloch equations, product operator matrix, and finite difference method. The simulated results reveal different diffusion behaviors of inter- and intra-molecular multiple-quantum coherences, coincident with theoretical predictions and experimental measurements. Compared with the Monte Carlo method, the finite difference method is more precise and efficient for simulating diffusion behaviors of multiple-quantum coherences.&lt;br /&gt;&lt;strong style="font-weight: normal;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/strong&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111886805903826717?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2005.03.126' title='Finite difference simulation of diffusion behaviors under inter- and intra-molecular multiple-quantum coherences in liquid NMR'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111886805903826717/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111886805903826717&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111886805903826717'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111886805903826717'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/06/finite-difference-simulation-of.html' title='Finite difference simulation of diffusion behaviors under inter- and intra-molecular multiple-quantum coherences in liquid NMR'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111815959108350870</id><published>2005-06-07T10:51:00.000-05:00</published><updated>2005-06-07T10:53:11.086-05:00</updated><title type='text'>Orientational dependence of intermolecular double quantum coherence (iDQC) signal from tendon tissue</title><content type='html'>Bahadir Ozus&lt;sup&gt;&lt;span style="font-size:-1;"&gt; &lt;/span&gt;&lt;/sup&gt;, Geoffrey D. Clarke&lt;sup&gt;&lt;span style="font-size:-1;"&gt; &lt;/span&gt;&lt;/sup&gt;, Stephen J. Dodd&lt;sup&gt;&lt;span style="font-size:-1;"&gt; &lt;/span&gt;&lt;/sup&gt;, Gary D. Fullerton&lt;sup&gt;&lt;span style="font-size:-1;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/sup&gt;The proton signal changes as the long axis of tendon tissue is rotated with respect to the main magnetic field (&lt;i&gt;B&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;). The orientational changes in the tendon signal obtained using the correlation spectroscopy revamped by asymmetric &lt;i&gt;z&lt;/i&gt;-gradient echo detection (CRAZED) sequence, which allows the effects of intermolecular dipolar interactions to be observed, were investigated and compared with the orientational changes of the signals produced using correlation spectroscopy (COSY), spin-echo (SE), and one-pulse sequences. The intermolecular double quantum coherence (iDQC) signal obtained using the CRAZED sequence showed a variation in the signal from tendon tissue, with sharper peaks and greater relative differences between minimum and maximum signal values compared to the variations in the signal obtained from the COSY, SE, and one-pulse sequences. This result is attributed to the orientational dependence of the transverse relaxation rate of single (SQC) and double (DQH) quantum coherences &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt; and &lt;i&gt;R&lt;/i&gt;&lt;sub&gt;2,2&lt;/sub&gt;, respectively. Magn Reson Med 53:1183-1186, 2005. © 2005 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111815959108350870?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.20436' title='Orientational dependence of intermolecular double quantum coherence (iDQC) signal from tendon tissue'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111815959108350870/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111815959108350870&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111815959108350870'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111815959108350870'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/06/orientational-dependence-of.html' title='Orientational dependence of intermolecular double quantum coherence (iDQC) signal from tendon tissue'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111652319332552905</id><published>2005-05-19T12:18:00.000-05:00</published><updated>2005-05-19T12:19:53.330-05:00</updated><title type='text'>Functional magnetic resonance imaging with intermolecular double-quantum coherences at 3 T</title><content type='html'>Andreas Schäfer, Thies H. Jochimsen, Harald E. Möller&lt;sup&gt;&lt;span style="font-size:-1;"&gt; &lt;/span&gt;&lt;/sup&gt;&lt;br /&gt;&lt;br /&gt;Functional magnetic resonance imaging (fMRI) based on the selection of intermolecular double-quantum coherences (iDQC) was performed with a standard birdcage coil at 3 T in a group of normal human volunteers. Suppression of spurious signal contributions from unwanted coherence-transfer pathways was achieved by combining a two-step phase cycle and a long repetition time of 5 s. A gradient-recalled echo iDQC sequence (echo time, &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;E&lt;/sub&gt; = 80 ms) yielded robust activation with a visual paradigm. Maximum &lt;i&gt;z&lt;/i&gt;-scores were about half of those observed with conventional blood-oxygen level dependent fMRI, whereas the functional signal change increased by more than a factor of 5. No activation was obtained with a spin-echo iDQC sequence (&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;E&lt;/sub&gt; = 160 ms), in which dephasing accumulated during the evolution period was fully rephased by an appropriate delay time. It is hypothesized that substantial inherent diffusion weighting of the iDQC technique efficiently suppresses intravascular contributions to the functional contrast. A consistent quantitative explanation of the observed amount of signal change currently remains speculative. Magn Reson Med 53:1402-1408, 2005. © 2005 Wiley-Liss, Inc.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111652319332552905?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.20506' title='Functional magnetic resonance imaging with intermolecular double-quantum coherences at 3 T'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111652319332552905/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111652319332552905&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111652319332552905'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111652319332552905'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/05/functional-magnetic-resonance-imaging.html' title='Functional magnetic resonance imaging with intermolecular double-quantum coherences at 3 T'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111618191175564097</id><published>2005-05-15T13:27:00.000-05:00</published><updated>2005-05-15T13:31:51.756-05:00</updated><title type='text'>Dipolar field effects described by boson operators techniques: The case of intermolecular multiple-quantum coherences in liquids</title><content type='html'>&lt;strong&gt;&lt;/strong&gt;W. Nosel, T. Gili, S. Capuani and  B. Maraviglia&lt;br /&gt;                   Chemical Physics Letters                                       &lt;br /&gt;   Volume 406, Issues 4-6           ,   2 May 2005,   Pages 452-456&lt;span style="font-size: smaller; font-family: Verdana;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;Dipolar couplings between macroscopically distant spins in solution nuclear magnetic resonance (NMR) are treated. We propose a novel technique to calculate the intermolecular multiple-quantum coherences (iMQCs) based on a boson operators approach. The choice of an annihilation and creation operator basis set allows us to produce a general expression of the NMR signal depending on local inhomogeneities of magnetic field. The general expression we derive fits into the well known background of iMQCs signal descriptions [J. Jeener, J. Chem. Phys. 112 (2000) 5091] and turns into the conventional quantum-mechanical Warren formulation [S. Lee, W. Richter, S. Vathyam, W.S. Warren, J. Chem. Phys. 105 (1996) 874] by means of appropriate approximations.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111618191175564097?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1016/j.cplett.2005.03.023' title='Dipolar field effects described by boson operators techniques: The case of intermolecular multiple-quantum coherences in liquids'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111618191175564097/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111618191175564097&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111618191175564097'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111618191175564097'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/05/dipolar-field-effects-described-by.html' title='Dipolar field effects described by boson operators techniques: The case of intermolecular multiple-quantum coherences in liquids'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111618162200114021</id><published>2005-05-15T13:24:00.000-05:00</published><updated>2005-05-15T13:27:02.006-05:00</updated><title type='text'>Application of a Fourier-based method for rapid calculation of field inhomogeneity due to spatial variation of magnetic susceptibility</title><content type='html'>J.P. Marques, R. Bowtell&lt;br /&gt;&lt;br /&gt;Inhomogeneous &lt;i&gt;B&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;-magnetic fields generate distortion in magnetic resonance images, particularly those produced using echo planar imaging, and are responsible for signal reduction due to intravoxel dephasing in gradient echo experiments. Such effects increase in magnitude in proportionality with the static field strength, and with the growing use of high-field (3 T and above) systems in medical imaging, it is increasingly important to be able to quantify field inhomogeneities. Here, we describe the implementation and use of a method for rapidly calculating frequency shifts due to spatially varying magnetic susceptibility that is based on an approach previously used to calculate long-range dipolar field effects. The method relies on a simple expression that relates the three-dimensional Fourier transforms of the magnetization distribution and the field, and can naturally include the effect of the sphere of Lorentz. It has been used to evaluate field inhomogeneity in the head due to the variation of magnetic susceptibility with tissue type and to calculate the change in field inhomogeneity that occurs due to small rotations of the head. In addition, this approach has been used to simulate the effect of lung volume changes in generating respiration induced resonant offsets in the brain. © Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 25B: 65-78, 2005&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111618162200114021?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/cmr.b.20034' title='Application of a Fourier-based method for rapid calculation of field inhomogeneity due to spatial variation of magnetic susceptibility'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111618162200114021/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111618162200114021&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111618162200114021'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111618162200114021'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/05/application-of-fourier-based-method.html' title='Application of a Fourier-based method for rapid calculation of field inhomogeneity due to spatial variation of magnetic susceptibility'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111532349364901585</id><published>2005-05-05T14:55:00.000-05:00</published><updated>2005-05-05T15:04:53.670-05:00</updated><title type='text'>ISMRM 2005 Abstracts on DDF/iMQC</title><content type='html'>Here are the DDF/iMQC related abstracts at ISMRM, &lt;a href="mailto:corum@cmrr.umn.edu"&gt;let me know&lt;/a&gt; if I missed any...&lt;br /&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02211.pdf"&gt;Quantitative Investigation of Rotating-Frame Intermolecular&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/01283.pdf"&gt;Simulation of Diffusion Behaviors under Scalar and Dipolar Couplings&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02348.pdf"&gt;Selection and Suppression of Intra- and Inter-Molecular MQCs&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02288.pdf"&gt;Investigation of multiple-echo spin-echo signal acquisition under distant dipole-dipole interactions&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02213.pdf"&gt;Issues and Artifacts in Intermolecular Double Quantum Imaging&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02362.pdf"&gt;Sensitivity enhancement in breast tumor imaging with MultiCRAZED experiments&lt;/a&gt;&lt;br /&gt;&lt;a href="http://cds.ismrm.org/ismrm-2005/Files/02210.pdf"&gt;Contrast Enhancement by the Butterfly Effect and Chaos Control in High-Field MRI&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;At the moment one needs their registration password to get to these links, this should change after the conference.&lt;br /&gt;&lt;br /&gt;Curt&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111532349364901585?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111532349364901585/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111532349364901585&amp;isPopup=true' title='1 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111532349364901585'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111532349364901585'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/05/ismrm-2005-abstracts-on-ddfimqc.html' title='ISMRM 2005 Abstracts on DDF/iMQC'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>1</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111306208898701611</id><published>2005-04-09T10:49:00.000-05:00</published><updated>2005-04-09T11:19:53.043-05:00</updated><title type='text'>LASER and iZQC meet at ENC...</title><content type='html'>&lt;A HREF="http://www.enc-conference.org/DisplayAbstractList2.aspx?Conf=ENC2005&amp;Session=P07" target="blank" &gt; session information  &lt;/A&gt;&lt;br /&gt;&lt;br /&gt;abstracts:&lt;br /&gt;&lt;A HREF="http://www.enc-conference.org/LongAbs/E050374.pdf" target="blank" &gt; Localized Intermolecular Zero-Quantum Coherence Spectroscopy in vivo  &lt;/A&gt;&lt;br /&gt;David Balla and Cornelius Faber&lt;br /&gt;&lt;br /&gt;&lt;A HREF="http://www.enc-conference.org/LongAbs/E050506.pdf" target="blank" &gt; First Results with "LASER" localized HOMOGENIZED sequence  &lt;/A&gt;&lt;br /&gt;Curtis A Corum and Michael Garwood&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111306208898701611?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111306208898701611/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111306208898701611&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111306208898701611'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111306208898701611'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/04/laser-and-izqc-meet-at-enc.html' title='LASER and iZQC meet at ENC...'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111211820681312842</id><published>2005-03-29T11:39:00.000-06:00</published><updated>2005-03-29T11:43:26.816-06:00</updated><title type='text'>Rotating-frame intermolecular double-quantum spin-lattice relaxation T1rho, DQC-weighted magnetic resonance imaging</title><content type='html'>Rotating-frame intermolecular double-quantum spin-lattice relaxation T1rho, DQC-weighted magnetic resonance imaging&lt;br /&gt;Bingwen Zheng, Dennis W. Hwang, Zhong Chen, Lian-Pin Hwang&lt;br /&gt;Magnetic Resonance in Medicine, Volume 53, Issue 4, p 930-936 (April 2005)&lt;br /&gt;http://dx.doi.org/10.1002/mrm.20432&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111211820681312842?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1002/mrm.20432' title='Rotating-frame intermolecular double-quantum spin-lattice relaxation T1rho, DQC-weighted magnetic resonance imaging'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111211820681312842/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111211820681312842&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111211820681312842'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111211820681312842'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/03/rotating-frame-intermolecular-double.html' title='Rotating-frame intermolecular double-quantum spin-lattice relaxation T1rho, DQC-weighted magnetic resonance imaging'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111134731050948400</id><published>2005-03-20T13:34:00.000-06:00</published><updated>2005-03-20T13:35:10.510-06:00</updated><title type='text'>Nonlinear Amplification of Small Spin Precession Using Long-Range Dipolar Interactions</title><content type='html'>&lt;dd&gt;M. P. Ledbetter, I. M. Savukov, and M. V. Romalis &lt;/dd&gt;&lt;br /&gt;&lt;a href="http://dx.doi.org/10.1103/PhysRevLett.94.060801"&gt;Nonlinear Amplification of Small Spin Precession Using Long-Range Dipolar Interactions&lt;/a&gt;&lt;br /&gt;Phys. Rev. Lett. &lt;b&gt;94&lt;/b&gt;, 060801 (2005)&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111134731050948400?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='related' href='http://dx.doi.org/10.1103/PhysRevLett.94.060801' title='Nonlinear Amplification of Small Spin Precession Using Long-Range Dipolar Interactions'/><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111134731050948400/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111134731050948400&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111134731050948400'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111134731050948400'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/03/nonlinear-amplification-of-small-spin.html' title='Nonlinear Amplification of Small Spin Precession Using Long-Range Dipolar Interactions'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-11580141.post-111134481173816108</id><published>2005-03-20T12:47:00.000-06:00</published><updated>2005-03-20T13:01:28.830-06:00</updated><title type='text'>DDF and iMQC News</title><content type='html'>First Post...&lt;br /&gt;&lt;br /&gt;DDF and iMQC Researchers,&lt;br /&gt;&lt;br /&gt;Here is an opportunity to share news, new publications, preprints, and comments with the community.&lt;br /&gt;&lt;br /&gt;Enjoy,&lt;br /&gt;&lt;br /&gt;Curt&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/11580141-111134481173816108?l=ddf-imqc.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://ddf-imqc.blogspot.com/feeds/111134481173816108/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://www.blogger.com/comment.g?blogID=11580141&amp;postID=111134481173816108&amp;isPopup=true' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111134481173816108'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/11580141/posts/default/111134481173816108'/><link rel='alternate' type='text/html' href='http://ddf-imqc.blogspot.com/2005/03/ddf-and-imqc-news.html' title='DDF and iMQC News'/><author><name>Curt</name><uri>http://www.blogger.com/profile/07473736537183652064</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry></feed>
