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th  - 1987 - 51st ENC Conference

th  - 1987 - 51st ENC Conference

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Monday - PM<br />

The NMR Gyro: An Application of NMR in a<br />

Slowly Rotating Frame<br />

Ann T. Nicol<br />

Litton Guidance and Control Systems<br />

5500 Canoga Avenue<br />

Woodland Hills, CA 91367<br />

The NMR gyro is a device which senses rotations <strong>th</strong>rough<br />

changes in frequency (or phase) of an NMR signal as a result of<br />

rotations relative to <strong>th</strong>e inertial precession of a nuclear<br />

magnetic moment. Mechanization of such a device requires <strong>th</strong>at<br />

<strong>th</strong>e entire NMR ',spectrometer" undergoes <strong>th</strong>e rotation and <strong>th</strong>at<br />

<strong>th</strong>is "spectrometer" be compact, occupying only a few cubic<br />

inches. This condition is realized in systems where a fairly<br />

high degree of nuclear polarization is achieved in very low<br />

fields (less <strong>th</strong>an I gauss). The approach uses isotopes of noble<br />

gases and <strong>th</strong>e nuclear polarization is achieved <strong>th</strong>rough a cross<br />

polarization wi<strong>th</strong> optically pumped alkalis. This presentation<br />

will discuss <strong>th</strong>e basic physical principles of <strong>th</strong>e NMR gyro and<br />

will present experimental results on <strong>th</strong>e processes and<br />

interactions governing nuclear polarization and relaxation in<br />

such systems.<br />

References<br />

I. A.T. Nicol, Phys. Rev. B 29, 2397 (1984).<br />

2. T.M. Kwon, J.G. Mark, and C.H. Volk, Phys. Rev A 24, 1894<br />

(1981).

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