Low-temperature transport, thermal, and optical properties of single-grain quasicrystals of icosahedral phases in the Y-Mg-Zn and Tb-Mg-Zn alloy systems

M. A. Chernikov, S. Paschen, E. Felder, P. Vorburger, B. Ruzicka, L. Degiorgi, H. R. Ott, I. R. Fisher, and P. C. Canfield
Phys. Rev. B 62, 262 – Published 1 July 2000
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Abstract

We present a comprehensive series of results of electrical transport (electrical conductivity, magnetoconductivity, Hall effect), thermal (specific heat), and optical (reflectivity) measurements in varying temperature ranges between 1.5 and 300 K on high-quality single-grain quasicrystals of icosahedral Y-Mg-Zn. This data set is augmented by the specific-heat and optical-reflectivity data obtained from a single-grain quasicrystal of icosahedral Tb-Mg-Zn. For Y-Mg-Zn, both the electrical conductivity σ(T) and magnetoconductivity δσ(H) may be described by calculations considering quantum interference effects. A detailed comparison of the weak-localization contributions to σ(T) and δσ(H) with our experimental data provides estimates of the inelastic and spin-orbit relaxation rates. The inelastic relaxation rate is found to be proportional to T3. The dominant contributions to the optical conductivity σ1(ω) spectrum, obtained from the reflectivity R(ω) data in the frequency range between 16 and 9.7×104cm1, are a strong Drude feature at low frequencies and a prominent absorption signal centered at approximately 6×103cm1. A comparison of the spectral weight of the Drude contribution to σ1(ω) with the magnitude of the linear-in-T term γT of the low-temperature specific heat Cp(T) yields the itinerant charge-carrier density ni=7.62×1021cm3 or 0.13 charge carriers per atom. The low ni value is corroborated by the results of the Hall effect measurements. For Tb-Mg-Zn, the optical conductivity σ1(ω) spectrum reveals features similar to those of Y-Mg-Zn. The low-temperature specific heat Cp(T) of Tb-Mg-Zn is strongly influenced by a spin-glass-type freezing of Tb moments and by crystal-electric-field effects.

  • Received 17 November 1999

DOI:https://doi.org/10.1103/PhysRevB.62.262

©2000 American Physical Society

Authors & Affiliations

M. A. Chernikov*, S. Paschen, E. Felder, P. Vorburger, B. Ruzicka, L. Degiorgi, and H. R. Ott

  • Laboratorium für Festkörperphysik, Eidgenössische Technische Hochschule-Zürich, 8093 Zürich, Switzerland

I. R. Fisher and P. C. Canfield

  • Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011

  • *Present address: Texas Center for Superconductivity, University of Houston, Houston, TX 77204.
  • Present address: Max-Planck-Institut für chemische Physik fester Stoffe, Nöthnitzerstrasse 48, 01187 Dresden, Germany.

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Vol. 62, Iss. 1 — 1 July 2000

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