Proton spin-lattice relaxation mechanisms and the metal-insulator transition in cerium hydrides
- 1 January 1984
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review B
- Vol. 29 (1) , 61-70
- https://doi.org/10.1103/physrevb.29.61
Abstract
Nuclear-magnetic-resonance (NMR) experiments have been done on cerium hydride () samples to search for correlations between NMR properties and known electrical conductivity changes as a function of hydrogen concentration and temperature. Data are presented for the spin-lattice relaxation rate and some line shapes for for temperatures from about 100 to 375 K. Although two resonances are observed at some temperatures, proton spin-lattice relaxation is characterized by a single relaxation time at each and . To a good approximation , where is attributed to direct dipolar coupling between protons and the electronic magnetic dipole moment of , and is an essentially temperature-independent term attributed to indirect [Ruderman-Kittel-Kasuya-Yosida (RKKY)] coupling to the moment. The term is so large that for most experiments the proton-proton dipolar and proton—conduction-electron couplings are negligible. The dependence of the constant is consistent with the dipolar coupling. The constant decreases in a steep manner as is increased above just below the regime , where the metal-semiconductor transition occurs in . It is proposed that and that the RKKY interaction includes coupling through the -band density of states. The marked decreases in and in the electrical conductivity that are associated with the concentration-dependent transition are thus attributed to the vanishing electron density of states at the Fermi surface. No temperature-dependent transition in is found. Results are consistent with a Mott transition model in which the electron donors are hydrogen vacancies.
Keywords
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