Detection and control of broken symmetries with Andreev bound state tunneling spectroscopy: effects of atomic-scale disorder

被引:4
作者
Greene, LH
Hentges, PJ
Aubin, H
Aprili, M
Badica, E
Covington, M
Pafford, MM
Westwood, G
Klemperer, WG
Jian, S
Hinks, DG
机构
[1] Univ Illinois, Dept Phys, Urbana, IL 61801 USA
[2] Univ Illinois, Fredrick Seitz Mat Res Lab, Urbana, IL 61801 USA
[3] Univ Illinois, Dept Chem, Urbana, IL 61801 USA
[4] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
来源
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS | 2004年 / 408卷
关键词
planar tunneling spectroscopy; Andreev bound states; broken time-reversal symmetry; unconventional superconductivity; high-temperature superconductivity;
D O I
10.1016/j.physc.2004.03.138
中图分类号
O59 [应用物理学];
学科分类号
摘要
Quasiparticle planar tunneling spectroscopy is used to study unconventional superconductivity in YBa2Cu3O7 (YBCO) thin films and BiSr2CaCu2O8 (BSCCO) single crystals. Tunneling conductances are obtained as a function of crystallographic orientation, applied magnetic field (magnitude and orientation), atomic substitution and surface damage. Our systematic studies confirm that the observed zero-bias conductance peak (ZBCP), a measure of the near-surface quasiparticle (QP) density of states (DoS), is comprised of Andreev bound states (ABS) resulting directly from the sign change of the d-wave order parameter (OP) at the Fermi surface. Our data, plus a literature search, reveals a consistency in the observation of the splitting of the ZBCP in optimally-doped materials. We note that the splitting of the ZBCP observed in applied field, and the spontaneous splitting observed at lower temperatures in zero field, occur concomitantly in a given junction, and that observation of this splitting is dependent upon two parameters: (1) the magnitude of the tunneling cone and (2) the degree of atomic-scale disorder at the interface. (C) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:804 / 806
页数:3
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