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th  - 1987 - 51st ENC Conference

th  - 1987 - 51st ENC Conference

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MF75<br />

NMR IMAGING USING CIRCULAR SIGNALS IN THE SPATIAL FREQU<strong>ENC</strong>Y DOMAIN S<br />

S. Matsul, K. Seklhara, and H. Kohno<br />

Central Research Laboratory, Hitachi, Ltd.<br />

P.O. Box 2, Kokubunji, Tokyo 185, Japan<br />

We demonstrate experlmentally a new type of me<strong>th</strong>od of imaging, in<br />

which siena1 measurements are taken during rotation of a field gradient.<br />

Detailed aspects of <strong>th</strong>e me<strong>th</strong>od will be discussed in connection wi<strong>th</strong><br />

unusual properties of <strong>th</strong>e observed slgnal.<br />

Generally, <strong>th</strong>e slgnal measured during <strong>th</strong>e gradient rotation traces<br />

a circle in <strong>th</strong>e spatlal frequency domain (so-called k space). I) Al<strong>th</strong>ough<br />

<strong>th</strong>e clrcular signal contains some information for imaging, it does not<br />

provide useful data <strong>th</strong>at can be systematlcally and efficiently process-<br />

ed to yield a spin image. This is because <strong>th</strong>e circle is not symmetric<br />

about <strong>th</strong>e origin of <strong>th</strong>e k space. However, if <strong>th</strong>e center of <strong>th</strong>e clrcle<br />

is approprlately shifted to <strong>th</strong>e k origin, useful data can be obtained.<br />

The resultant signal directly provides symmetric circular phase infor-<br />

mation. The shift can be achieved by applying, amon E many ways, a sta-<br />

tionary fleld gradient prior to <strong>th</strong>e rotation. The properties of such<br />

a circular signal are completely different from <strong>th</strong>ose of a usual FID<br />

slgnal. The unusual properties can be understood by expressing <strong>th</strong>e<br />

clrcular signal in terms of Bessel functions of <strong>th</strong>e first kind.<br />

The radius of <strong>th</strong>e circle is given by 7G/WG, where Y is <strong>th</strong>e gyromag-<br />

netic ratio, G denotes <strong>th</strong>e gradient amplitude, and ~G is <strong>th</strong>e angular<br />

frequency of <strong>th</strong>e gradient rotation. Therefore, takin E measurements<br />

after changing ei<strong>th</strong>er <strong>th</strong>e gradient amplitude or <strong>th</strong>e angular frequency<br />

permits a concentric set of clrcular signals wi<strong>th</strong> different radii to<br />

be obtained. The signal set can be converted to a spin image by suit-<br />

able data processing involving Fourier transformations along <strong>th</strong>e radii<br />

and back projections.<br />

Reference<br />

I) S. Ljunggren, J. Magn. Reson. 54, 338 (1983).<br />

§ Published in part: S. Matsui and H. Kohno, J. Magn. Reson. 70, 157<br />

(1986).

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