Low-temperature H-1 nuclear magnetic resonance study of crystal and electronic structures of the nearly stoichiometric yttrium dihydride




Zogal OJ, Vuorimaki AH, Ylinen EE

PublisherTAYLOR & FRANCIS LTD

2000

Philosophical Magazine A: Physics of Condensed Matter, Structure, Defects and Mechanical Properties

PHILOSOPHICAL MAGAZINE A-PHYSICS OF CONDENSED MATTER STRUCTURE DEFECTS AND MECHANICAL PROPERTIES

PHILOS MAG A

80

11

2549

2558

10

0141-8610

DOIhttps://doi.org/10.1080/01418610008216491



Proton nuclear magnetic resonance absorption spectra and spin-lattice relaxation rates in yttrium dihydride have been measured in the temperature range from 4.2 to 310 K at 36.0 MHz. The second moment of the resonance line corresponds to the rigid-lattice regime for YH1.99 and its value agrees with the anticipated CaF2 type of structure. The main contribution to the spin-lattice relaxation rate R-1 arises from conduction electrons and is characterized by R-1e = 2.77 x 10(-3) s(-1) K-1 x T. Evidence of proton self-diffusion was seen in the linewidth and in R-1 for YH1.99+0.1 The onset temperature, about 250 K, of the self-diffusion, is close to the metal-semiconductor transition reported earlier for that hydride. Below that temperature the linewidth becomes temperature independent and the second moment of the line is explained in terms of different structure models. The fit to the temperature dependence of R-1 in the temperature range 70-310 K gives R-1e = 2.1 x 10(-3) s(-1) K-1 x T. The relaxation becomes almost temperature independent below 50 K. Various mechanisms for this behaviour are discussed. In addition, the R-1 data for the sample prepared with yttrium of 99.9% purity are presented. In contrast with the previous case, where pure yttrium from the Ames Laboratory was used, R-1 has a large contribution of spin diffusion to the paramagnetic Gd3+ ions.



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