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Electronic transport in insulating AlPdRe quasicrystals

Ralph Rosenbaum et al 2004 J. Phys.: Condens. Matter 16 821-831   doi: 10.1088/0953-8984/16/6/012  Help

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Ralph Rosenbaum1, Tim Murphy2, Bruce Brandt2, Chang-Ren Wang3, Yuan-Liang Zhong4, Shr-Wen Wu5, Shui-Tien Lin5 and Juhn-Jong Lin6
1 School of Physics and Astronomy, Tel Aviv University, Raymond and Beverly Sackler Faculty of Exact Sciences, Ramat Aviv 69978, Israel
2 National High Magnetic Field Laboratory, 1800 East Paul Dirac Drive, Tallahassee,FL 32310, USA
3 Department of Physics, Tunghai University, Taichung, Taiwan
4 Institute of Physics, Academia Sinica, 115 Taipei, Taiwan
5 Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan
6 Institute of Physics, National Chiao Tung University, Hsinchu 300, Taiwan
E-mail: ralphr@post.tau.ac.il

Abstract. Resistivity and magnetoresistance measurements have been performed on insulating icosahedral AlPdRe quasicrystal (QC) bar samples. At temperatures in the range 300\ntilde {\mathrm {K}} \ge T \ge 50\ntilde {\mathrm {K}} , the resistivities follow a simple inverse temperature law: ρ(T) = ρ0/T(1.0 ± 0.1). Below 1 K, the resistivity of a weakly insulating sample exhibited a simple inverse temperature law where ρ(T) = ρ0/T0.33 and not an activated variable-range hopping (VRH) law. Strongly insulating samples exhibit saturation of their resistivities to finite values as T \to 0\ntilde {\mathrm
{K}} . These saturation resistivity values are believed to arise from the presence of a second metallic phase located within the quasicrystal's structure. By extrapolating the measured resistivities at 22 mK to absolute zero, the saturation conductivity values were estimated at T = 0 K and subtracted from the conductivity data points. These 'corrected' data, corresponding only to the QC phase, were found to follow activated VRH laws, having hopping exponents y that vary in the range 0.18 \le y \le 0.43 . The activated VRH behaviours are observed only below 1 K. The magnetoresistances (MRs) of these samples are also anomalous. The MRs can be explained by including contributions from both the saturation conductivity values and from the QC MR ratios, estimated using the wavefunction shrinkage model.

Print publication: Issue 6 (18 February 2004)
Received 8 December 2003
Published 30 January 2004

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