Superconductivity and Charge Density Wave in ZrTe3−xSex

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作者
Xiangde Zhu
Wei Ning
Lijun Li
Langsheng Ling
Ranran Zhang
Jinglei Zhang
Kefeng Wang
Yu Liu
Li Pi
Yongchang Ma
Haifeng Du
Minglian Tian
Yuping Sun
Cedomir Petrovic
Yuheng Zhang
机构
[1] High Magnetic Field Laboratory,Condensed Matter Physics and Materials Science Department
[2] Chinese Academy of Sciences and University of Science and Technology of China,undefined
[3] Brookhaven National Laboratory,undefined
[4] Key Laboratory of Materials Physics,undefined
[5] Institute of Solid State Physics Chinese Academy of Sciences,undefined
[6] Collaborative Innovation Center of Advanced Microstructures,undefined
[7] School of Materials Science and Engineering,undefined
[8] Tianjin University of Technology,undefined
[9] Present address: CNAM,undefined
[10] Department of Physics,undefined
[11] University of Maryland,undefined
[12] College Park,undefined
[13] Maryland 20742,undefined
[14] USA.,undefined
[15] Present address: Condensed Matter Physics and Materials Science Department,undefined
[16] Upton NY 11973,undefined
[17] USA,undefined
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摘要
Charge density wave (CDW), the periodic modulation of the electronic charge density, will open a gap on the Fermi surface that commonly leads to decreased or vanishing conductivity. On the other hand superconductivity, a commonly believed competing order, features a Fermi surface gap that results in infinite conductivity. Here we report that superconductivity emerges upon Se doping in CDW conductor ZrTe3 when the long range CDW order is gradually suppressed. Superconducting critical temperature Tc(x) in ZrTe3−xSex (0 ≤ x ≤ 0.1) increases up to 4 K plateau for 0.04 ≤ x ≤ 0.07. Further increase in Se content results in diminishing Tc and filametary superconductivity. The CDW modes from Raman spectra are observed in x = 0.04 and 0.1 crystals, where signature of ZrTe3 CDW order in resistivity vanishes. The electronic-scattering for high Tc crystals is dominated by local CDW fluctuations at high temperatures, the resistivity is linear up to highest measured T = 300 K and contributes to substantial in-plane anisotropy.
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