ELECTRON-PARAMAGNETIC-RESONANCE SPECTRA OF NI2-DOPED ZN(BF4)2-CENTER-DOT-6H2O - TEMPERATURE AND CONCENTRATION-DEPENDENCE()

Citation
W. Sano et al., ELECTRON-PARAMAGNETIC-RESONANCE SPECTRA OF NI2-DOPED ZN(BF4)2-CENTER-DOT-6H2O - TEMPERATURE AND CONCENTRATION-DEPENDENCE(), Physical review. B, Condensed matter, 50(5), 1994, pp. 2958-2962
Citations number
16
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
50
Issue
5
Year of publication
1994
Pages
2958 - 2962
Database
ISI
SICI code
0163-1829(1994)50:5<2958:ESONZ>2.0.ZU;2-T
Abstract
The single-ion spin Hamiltonian parameters have been determined for zi nc fluoroborate hexahydrate doped with Ni2+ (3d8, S = 1) and compared with those obtained for nickel fluoroborate hexahydrate. To account fo r the differences observed, EPR for several concentrations (x = 0.005 to 1) was studied from room to liquid-helium temperature. Between 4.2 and 1.5 K, for low doping, they are constant with g(parallel-to) = 2.2 29 +/- 0.006, g(perpendicular-to) = 2.261 +/- 0.025, and D = - (0.1291 +/- 0.0008) cm-1. Appropriate values for nickel fluoroborate are near ly the same but they are weakly temperature dependent, attributed to a ferromagnetic interaction. At higher temperatures these parameters ar e remarkably concentration dependent. Two main lines arise in parallel orientation. For concentrations up to x almost-equal-to 0.04 and at 7 7 K, they show asymmetrically distributed satellite lines outside the more intense central portion. The satellite lines seem to increase wit h concentration but only those assigned to a ferromagnetic-coupled fir st-neighbor pair survive the simultaneous broadening effect. As the br oadening is asymmetric, the lines' centers shift smoothly outwards. At x almost-equal-to 0.7, we observe maximum broadening; for larger x no structural detail is seen and the spectra are progressively exchange narrowed. At the same time, the two lines are drawn together. The line width dependence on concentration indicates that the Ni ions have rand omly occupied the Zn sites as expected, and that the contribution from spin-lattice relaxation practically does not change with concentratio n. We conclude that the differences in the spin Hamiltonian parameters are due essentially to magnetic interactions throughout the whole tem perature range.