th - 1987 - 51st ENC Conference
th - 1987 - 51st ENC Conference
th - 1987 - 51st ENC Conference
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WF58<br />
SPATIAL LOCALISATION OF ~lp ~LR SPECTROSCOPY USING PHASE<br />
MODULATED ROTATING FRAI~E IMAGING.<br />
Kartin J. Blackledse*, Peter Styles and Georse K. Radda<br />
X.R.C. CLINICAL NAGNETIC RESONANCE FACILITY, JOHN RADCLIFFE HOSPITAL,<br />
OXFORD ENGLAND U.K.<br />
Rotating frame imaging (R.F.I.) using <strong>th</strong>e B, field gradient of a<br />
surface coil has been shown to be a viable me<strong>th</strong>od for localislng<br />
phosphorus spectra in-vivo. Use of separate coils for transmitting and<br />
receivin E signal ensures <strong>th</strong>at <strong>th</strong>e encoding field gradient is linear and<br />
<strong>th</strong>e shape of <strong>th</strong>is field <strong>th</strong>roughout <strong>th</strong>e interrogated resion is flat and<br />
planar. As normally implemented, R.F.I. is an inherently inefficient<br />
technique; <strong>th</strong>is is because <strong>th</strong>e observation pulse is incremented, and<br />
received signal is amplitude modulated wi<strong>th</strong> respect to incremental<br />
pulse ansle. The magnetisatlon precesses about <strong>th</strong>e x-axis of <strong>th</strong>e<br />
rotatin 5 frame_, so <strong>th</strong>at of <strong>th</strong>e two components (y and z), only <strong>th</strong>e y<br />
component is detected. To overcome <strong>th</strong>is insensitivity, it i$ necessary<br />
to detect <strong>th</strong>e z component. This is achieved by 'flipping' <strong>th</strong>e<br />
masnetisation, immediately after <strong>th</strong>e incremental pulse, into <strong>th</strong>e x-y<br />
plane usin 5 a 7/2 pulse applied alon E <strong>th</strong>e y axis This signal is phase<br />
modulated, <strong>th</strong>e relative x and y component masnetisation in <strong>th</strong>e rotatin$<br />
frame varies wi<strong>th</strong> pulse angle. For <strong>th</strong>is modulation to be useful, <strong>th</strong>e<br />
phase encoding pulse (p.e.p) is required to have a bandwid<strong>th</strong> in bo<strong>th</strong><br />
B, and Bo over which it is effective in accurately transposln8 <strong>th</strong>e<br />
phase of <strong>th</strong>e mnsnetisation vector from <strong>th</strong>e y-z to <strong>th</strong>e x-y plane.<br />
Usin 5 a double coil (wi<strong>th</strong> smaller receiver coil) we receive from <strong>th</strong>e<br />
region (.2-.8) radii of <strong>th</strong>e transmitter coil away from <strong>th</strong>e surface. In<br />
<strong>th</strong>is resion, <strong>th</strong>e B, field streng<strong>th</strong> varies from >.5 to