Abstract
AbstractA longitudinal spin‐lattice relaxation time T1 is considered for conduction electrons due to optical phonons scattering in a high magnetic field. The temperature and field dependences of T1 are obtained for the quantum limit and for various mutual locations of the Fermi level and the two lowest spin sublevels of the carriers. It is shown that the deviation of the phonon distribution from thermal equilibrium due to the interaction with the spins of the conduction electrons is small, and a phonon bottleneck should not occur, in contrast with the case of spin‐lattice relaxation of localized spins.
References
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Dates
Type | When |
---|---|
Created | 18 years, 1 month ago (July 9, 2007, 6:09 p.m.) |
Deposited | 1 year, 10 months ago (Oct. 19, 2023, 12:44 p.m.) |
Indexed | 1 year, 8 months ago (Nov. 23, 2023, 6:15 p.m.) |
Issued | 58 years, 7 months ago (Jan. 1, 1967) |
Published | 58 years, 7 months ago (Jan. 1, 1967) |
Published Online | 19 years, 4 months ago (March 30, 2006) |
Published Print | 58 years, 7 months ago (Jan. 1, 1967) |
@article{Kalashnikov_1967, title={Theory of Spin‐Lattice Relaxation of Conduction Electrons of Ionic Semiconductors at Extremely High Magnetic Fields}, volume={21}, ISSN={1521-3951}, url={http://dx.doi.org/10.1002/pssb.19670210239}, DOI={10.1002/pssb.19670210239}, number={2}, journal={physica status solidi (b)}, publisher={Wiley}, author={Kalashnikov, V. P.}, year={1967}, month=jan, pages={775–784} }