Magnetism and transport properties of HfMSi (M = PT, Pd) and HfRh1-xPdxSi

Citation
S. Yashiro et al., Magnetism and transport properties of HfMSi (M = PT, Pd) and HfRh1-xPdxSi, J ALLOY COM, 298(1-2), 2000, pp. 51-58
Citations number
13
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF ALLOYS AND COMPOUNDS
ISSN journal
09258388 → ACNP
Volume
298
Issue
1-2
Year of publication
2000
Pages
51 - 58
Database
ISI
SICI code
0925-8388(20000228)298:1-2<51:MATPOH>2.0.ZU;2-0
Abstract
The crystallographic, electric, and magnetic properties of the new intermet allic compounds HfMSi (M = Pt or Pd) and the superconductivity of HfRh1-xPd xSi were studied. The crystal structure of HfPtSi and HfPdSi could be refin ed assuming an orthorhombic structure (space group Pnma) and lattice consta nts of a = 0.6549 nm, b = 0.3883 nm, and c = 0.7505 nm for HfPtSi and a = 0 .6570 nm, b = 0.3874 nm, and c = 0.7565 nm for HfPdSi. Both compounds are m etallic and show diamagnetic behavior below 300 K. A small effective electr on mass is thought to be a reason for the diamagnetism of HfMSi (M = Pt or Pd). In the HfRh1-xPdxSi system, the superconductivity of HfRhSi (T-c = 2.2 K) is suppressed by replacing Ph by Pd. The Pd content dependence of the P auli paramagnetic susceptibility suggests that reduction of the density of states at the Fermi level is a possible cause of the suppression of superco nductivity in the HfRh1-xPdxSi system. (C) 2000 Published by Elsevier Scien ce S.A. AU rights reserved.