## Abstract Spin‐lattice relaxation mechanisms of nuclear spins in solids in the presence of low concentrations of paramagnetic centers are discussed. Apart from the electron spin‐lattice relaxation mechanism, three‐spin processes involving two electron spins and a nuclear spin may also play a role
Spin-lattice relaxation of spin-½ nuclei in solids containing diluted paramagnetic impurity centers. II. Dynamic polarization of nuclear spin system by thermal mixing and solid-state effect
✍ Scribed by E.C. Reynhardt
- Publisher
- John Wiley and Sons
- Year
- 2003
- Tongue
- English
- Weight
- 237 KB
- Volume
- 19A
- Category
- Article
- ISSN
- 1546-6086
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✦ Synopsis
Abstract
Dynamic nuclear polarization of nuclear spins via the solid‐state and thermal mixing effects is discussed. Continuous‐wave S‐ and X‐band microwave radiation have been employed to measure ^13^C signal enhancements and polarization times for ^13^C nuclei in a natural type Ib diamond as a function of magnetic field. It was found that thermal mixing plays an important role in the ^13^C signal enhancement because the central electron spin resonance (ESR) line width H~L~ ≃ H~0~γ~C~/γ~e~, resulting in flip‐flip and flip‐flop forbidden transitions taking place simultaneously. On the other hand, the ^13^C spin‐lattice relaxation rate is determined to a large extent by the solid‐state effect (forbidden transitions). ^13^C polarization rates have also been measured for a suite of natural diamonds. It is shown that the polarization rate is proportional to the paramagnetic impurity concentration, in agreement with the theory. © 2003 Wiley Periodicals, Inc. Concepts Magn Reson 19A: 36–43, 2003.
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