Proton spin-lattice relaxation mechanisms and the metal-insulator transition in cerium hydrides

Abstract
Nuclear-magnetic-resonance (NMR) experiments have been done on cerium hydride (CeHx) 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 H1 spin-lattice relaxation rate R1 (=1T1) and some line shapes for 2.10x2.92 for temperatures from about 100 to 375 K. Although two H1 resonances are observed at some temperatures, proton spin-lattice relaxation is characterized by a single relaxation time at each x and T. To a good approximation R1=AT+R, where AT is attributed to direct dipolar coupling between protons and the electronic magnetic dipole moment of Ce3+, and R is an essentially temperature-independent term attributed to indirect [Ruderman-Kittel-Kasuya-Yosida (RKKY)] coupling to the Ce3+ moment. The AT term is so large that for most experiments the proton-proton dipolar and proton—conduction-electron couplings are negligible. The x dependence of the constant A is consistent with the dipolar coupling. The constant R decreases in a steep manner as x is increased above x2.65 just below the regime 2.75<x<2.85, where the metal-semiconductor transition occurs in CeHx. It is proposed that RNd(EF) and that the RKKY interaction includes coupling through the d-band density of states. The marked decreases in R1 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 R1 is found. Results are consistent with a Mott transition model in which the electron donors are hydrogen vacancies.