Two-Channel Kondo Physics due to As Vacancies in the Layered Compound ZrAs1.58Se0.39

被引:22
作者
Cichorek, T. [1 ]
Bochenek, L. [1 ]
Schmidt, M. [2 ]
Czulucki, A. [2 ]
Auffermann, G. [2 ]
Kniep, R. [2 ]
Niewa, R. [3 ]
Steglich, F. [2 ,4 ,5 ]
Kirchner, S. [4 ]
机构
[1] Polish Acad Sci, Inst Low Temp & Struct Res, PL-50950 Wroclaw, Poland
[2] Max Planck Inst Chem Phys Solids, D-01187 Dresden, Germany
[3] Univ Stuttgart, Inst Inorgan Chem, D-70569 Stuttgart, Germany
[4] Zhejiang Univ, Ctr Correlated Matter, Hangzhou 310058, Zhejiang, Peoples R China
[5] Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
基金
美国国家科学基金会; 中国国家自然科学基金;
关键词
TUNNELING CENTERS; METALLIC GLASSES; AMORPHOUS METALS; 2-LEVEL SYSTEMS; STATE; SUPERCONDUCTOR; TEMPERATURE; FLUCTUATION; IMPURITIES; RESISTANCE;
D O I
10.1103/PhysRevLett.117.106601
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We address the origin of the magnetic-field-independent -vertical bar A vertical bar T-1/2 term observed in the low-temperature resistivity of several As-based metallic systems of the PbFCl structure type. For the layered compound ZrAs1.58Se0.39, we show that vacancies in the square nets of As give rise to the low-temperature transport anomaly over a wide temperature regime of almost two decades in temperature. This low-temperature behavior is in line with the nonmagnetic version of the two-channelKondo effect, whose origin we ascribe to a dynamic Jahn-Teller effect operating at the vacancy-carrying As layer with a C-4 symmetry. The pair-breaking nature of the dynamical defects in the square nets of As explains the lowsuperconducting transition temperature T-c approximate to 0.14 K of ZrAs1.58Se0.39 compared to the free-of-vacancies homologue ZrP1.54S0.46 (T-c approximate to 3.7 K). Our findings should be relevant to a wide class of metals with disordered pnictogen layers.
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页数:6
相关论文
共 48 条
[1]  
ABRIKOSOV AA, 1961, SOV PHYS JETP-USSR, V12, P1243
[2]  
Akkermans E., 2006, MESOSCOPIC PHYS ELEC
[3]   Nonexistence of a strong coupling two-channel Kondo fixed point for microscopic models of tunneling centers [J].
Aleiner, IL ;
Controzzi, D .
PHYSICAL REVIEW B, 2002, 66 (04) :451071-4510715
[4]   Kondo temperature for the two-channel Kondo models of tunneling centers [J].
Aleiner, IL ;
Altshuler, BL ;
Galperin, YM ;
Shutenko, TA .
PHYSICAL REVIEW LETTERS, 2001, 86 (12) :2629-2632
[5]  
Altshuler B. L., 1985, ELECT ELECT INTERACT
[6]  
[Anonymous], 1993, TheKondo Problem to Heavy Fermions
[7]   Stable two-channel kondo fixed point of an SU(3) quantum defect in a metal: Renormalization-group analysis and conductance spikes [J].
Arnold, Michael ;
Langenbruch, Tobias ;
Kroha, Johann .
PHYSICAL REVIEW LETTERS, 2007, 99 (18)
[8]  
Binnewies M, 2012, CHEMICAL VAPOR TRANSPORT REACTIONS, P1, DOI 10.1515/9783110254655
[9]   Extended Two-Channel Kondo Phase of a Rotational Quantum Defect in a Fermi Gas [J].
Chuo, E. Fuh ;
Ballmann, K. ;
Borda, L. ;
Kroha, J. .
27TH INTERNATIONAL CONFERENCE ON LOW TEMPERATURE PHYSICS (LT27), PTS 1-5, 2014, 568
[10]   Two-channel Kondo effect in glasslike ThAsSe [J].
Cichorek, T ;
Sanchez, A ;
Gegenwart, P ;
Weickert, F ;
Wojakowski, A ;
Henkie, Z ;
Auffermann, G ;
Paschen, S ;
Kniep, R ;
Steglich, F .
PHYSICAL REVIEW LETTERS, 2005, 94 (23)