th - 1987 - 51st ENC Conference
th - 1987 - 51st ENC Conference
th - 1987 - 51st ENC Conference
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WK3S<br />
EXPERIMENTAL STUDY OF THE OPTIRIZED SELECTIVE RF PULSES<br />
Jintong Haoo, T.H. hreci, K.E. Scott and E.R. Andrev<br />
Departments of Radiology and Physics<br />
Gsinesvllle, FL 32611<br />
Selective rodiofrequency (rf) pulmes ore important in bo<strong>th</strong> NHR<br />
spectroscopy end imaging. Because <strong>th</strong>e magnetization equation of<br />
motion is nonlineor, <strong>th</strong>e design of <strong>th</strong>e rf pulse shapes cspoble of<br />
precisely affecting <strong>th</strong>e magnetization in a veil-defined frequency<br />
range is not s simple problem. Recently, <strong>th</strong>e concept of optimal<br />
control hob been introduced for <strong>th</strong>e design of rf pulses amplitude<br />
modulated as a function of time to provide frequency selectivity.<br />
Several selective pulse shapes hsve been developed using <strong>th</strong>ese<br />
te<strong>th</strong>ods, hoverer, very few experimental results have been presented.<br />
We have presented a detoiled description of <strong>th</strong>e use of <strong>th</strong>e conjugate<br />
gradient me<strong>th</strong>od in <strong>th</strong>e optics1 control problem to design a selective<br />
180 degree inversion pulses (1). Using <strong>th</strong>is me<strong>th</strong>od, we have found a<br />
series of <strong>th</strong>e 9e and <strong>th</strong>e 180 degree rf pulse shapes <strong>th</strong>at have very<br />
high selectivity. We have performed experiments on I GE CS1-2<br />
imager/spectrometer vhich confirm <strong>th</strong>eoretical predictions from <strong>th</strong>e<br />
application of optimal control me<strong>th</strong>ods. Bo<strong>th</strong> our computer<br />
simulations end experimental results are presented in <strong>th</strong>is poster.<br />
Also, we 8how <strong>th</strong>at <strong>th</strong>e frequency response of <strong>th</strong>e magnetization<br />
affected by a selective 180 degree inversion rf pulse is <strong>th</strong>e game as<br />
<strong>th</strong>at for a selective refocusing pulse. Computer simulations for bo<strong>th</strong><br />
a sinc and optimal pulse are presented to demonstrate <strong>th</strong>e principle<br />
and experimental results for selective refocusing pulses ire<br />
presented. Thus, I single optimal selective 180 degree rf pulse can<br />
be used is ei<strong>th</strong>er in inversion or refocusing pulse. In bo<strong>th</strong><br />
IituationI, its selectivity can be optiIlzed to fit <strong>th</strong>e desired<br />
frequency profile end we rill diicuII how to apply <strong>th</strong>lI procedure in<br />
designing selective pulses to fit various selectivity criteria.<br />
Optimal control me<strong>th</strong>ods can also be applied to <strong>th</strong>e case of<br />
selective 90 degree rf pulses. The degree of improvement possible is<br />
not as great as for selective 180 degree pulses but significant<br />
improvement is possible. Bo<strong>th</strong> experimental and computer simulation<br />
results of <strong>th</strong>e optimal selective 90 degree rf pulses will also<br />
be presented in <strong>th</strong>is poster. Thus, <strong>th</strong>e optimal control se<strong>th</strong>od has<br />
solved <strong>th</strong>e problem of designing optimized rf pulse shapes for<br />
frequency selective excitation.<br />
This research is supported by grants from <strong>th</strong>e National Znstitute of<br />
Heal<strong>th</strong> {P41-RR-e2278) and <strong>th</strong>e Veterans Administration Medical<br />
Research Service.<br />
1. Jintong Meo, T. H. Mareci, K. N. Scott and E. R. Andrev, J. MIgn.<br />
ReIon. 70, 31e (1986)