th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
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-- 182 I<br />
SUPPRESSION OF ARTIFACTS<br />
IN MULTIPLE ECHO NUCLEAR MAGNETIC RESONANCE<br />
G.J.Barker*, T.H.Mareci.<br />
Department of Radiology,<br />
University of Florida, Gainesville, FL 32610.<br />
Many techniques in bo<strong>th</strong> Magnetic Resonance Imaging (MRI) and<br />
Magnetic Resonance Spectrosopy (MRS) use two or more rf pulses to ex-<br />
cite <strong>th</strong>e spin system and detect <strong>th</strong>e echo signals which form between or<br />
after <strong>th</strong>e pulses. After <strong>th</strong>e initial excitation <strong>th</strong>e evolution of <strong>th</strong>e<br />
spin system depends upon relaxation times, exchange rates, diffusion<br />
constants and o<strong>th</strong>er properties, wi<strong>th</strong> <strong>th</strong>e dominant mechanisms being<br />
determined by <strong>th</strong>e details of <strong>th</strong>e timing and tip angles of <strong>th</strong>e pulses.<br />
In general many different echoes form during each acquisition inter-<br />
val, one of which carries <strong>th</strong>e information required. The o<strong>th</strong>ers lead to<br />
distortion of peak heights and line shapes in MRS, and to ghost images<br />
and similar artifacts in MRI.<br />
The 'coherence transfer pa<strong>th</strong>way' formalism (1) allows <strong>th</strong>e evo-<br />
lution of each echo to be studied and suggests me<strong>th</strong>ods of removing <strong>th</strong>e<br />
unwanted signals. Phase cycling schemes haye been investigated which<br />
cause cancellation of <strong>th</strong>e unwanted echoes, in certain cases during a~l<br />
acquisition intervals of a multiple echo sequence. Such schemes re ~<br />
qulre a large number of transients to be collected, however, so a<br />
second me<strong>th</strong>od has been developed whereby <strong>th</strong>e systematic application of<br />
magnetic field gradients produce similar results wi<strong>th</strong>in a single tran-<br />
sient. Examples of <strong>th</strong>e a~plication of bo<strong>th</strong> me<strong>th</strong>ods to <strong>th</strong>e spin echo<br />
and TART (2) sequences In Imaglng, and to RED NOES¥ (3) in spectros =<br />
copy, show <strong>th</strong>eir success in remove artifacts.<br />
This research was supported in part by NIH Biotechnology<br />
Resource Grant (P41-RR-02278) and <strong>th</strong>e Veteran Administration<br />
Medical Research Service.<br />
(1) G.Bodenhausen et al. , J. Magn. Reson. 58, 370, (1984)<br />
(2) T.H.Mareci et al. , J. Magn. Reson. 67, 55, (1986)<br />
(3) T.H.Mareci et a]. : 27<strong>th</strong> RNC_ R~]t~mn~A (lqR~%<br />
--183 I<br />
QUANTITATION OF EXCHANGE RATES<br />
USING THE RED NOESY SEQU<strong>ENC</strong>E<br />
M.D. Cockman* and T.H. Mareci<br />
Departments of Chemistry, Radiology, and Physics<br />
University of Florida, Gainesville, FL 32610.<br />
We have previously introduced <strong>th</strong>e RED NOESY pulse sequence<br />
for <strong>th</strong>e simultaneous acquisition of several 2D NOESY spectra, each<br />
wi<strong>th</strong> a different mixing time (i). The RED NOESY sequence is similar<br />
to <strong>th</strong>e NOESY sequence but <strong>th</strong>e final 90 degree pulse of <strong>th</strong>e latter is<br />
replaced by a series of "read" pulses of tip angles less <strong>th</strong>an 90 de-<br />
grees to sample <strong>th</strong>e exchanging longitudinal magnetization. This is<br />
<strong>th</strong>e same principle behind <strong>th</strong>e TART and STEAM T1 imaging sequences<br />
(2,3). Recently, Meyerhoff, et.al, have applied <strong>th</strong>e sequence to a<br />
small lactone and report good success in routlne use of <strong>th</strong>e pulse se-<br />
quence for <strong>th</strong>e observation of NOEs (4). We have investigated <strong>th</strong>e use<br />
of RED NOESY for <strong>th</strong>e quantitation of exchange rates for <strong>th</strong>ree small<br />
N,N-dime<strong>th</strong>[lamides. The most limiting aspects of RED NOESY are: i)<br />
<strong>th</strong>at <strong>th</strong>e slgnal acquisition time imposes a lower bound on <strong>th</strong>e mixing<br />
times and 2) <strong>th</strong>at <strong>th</strong>e read pulses form unwanted echoes. We present a<br />
homospoiling scheme designed to overcome <strong>th</strong>e second factor and exam-<br />
ine <strong>th</strong>e implications of <strong>th</strong>e first.<br />
This research was supported in part by <strong>th</strong>e NIH Biotechnology<br />
Resource Grant (P41-RR-02278) and <strong>th</strong>e Veterans Administration Medical<br />
Research Service.<br />
(I) T.H. Mareci, S. Donstrup, and M.D. Cockman, 27<strong>th</strong> <strong>ENC</strong>, Baltimore,<br />
1986.<br />
(2) T.H. Mareci, W. Sattin, K.N. Scott, and A. Bax, J. Magn. Reson,<br />
67, 55 (1986).<br />
(3) A. Haase and J. Frahm, J. Magn. Reson. 65, 481 (1986).<br />
(4) D.J. Meyerhoff, R. Nunlist, and J.F. O'Connell, Magn. Reson.<br />
Chem., 843, Oct (1987).<br />
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