Theory of magnetotunneling spectroscopy in spin triplet p-wave superconductors

被引:52
作者
Tanaka, Y [1 ]
Tanuma, Y
Kuroki, K
Kashiwaya, S
机构
[1] Nagoya Univ, Dept Appl Phys, Nagoya, Aichi 4648063, Japan
[2] JST, Crest, Nagoya, Aichi 4648063, Japan
[3] Okayama Univ, Grad Sch Nat Sci & Technol, Okayama 7008530, Japan
[4] Univ Electrocommun, Dept Appl Phys & Chem, Chofu, Tokyo 1828585, Japan
[5] Nat Inst Adv Ind Sci & Technol, Tsukuba, Ibaraki 3058568, Japan
关键词
triplet superconductor; tunneling conductance; Doppler shift; chirality;
D O I
10.1143/JPSJ.71.2102
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We study the influence of a magnetic field H on the zero bias conductance peak (ZBCP) due to zero energy Andreev bound states (ZES) in a normal metal/unconventional superconductor. For p-wave junctions, ZBCP does not split into two by H even for sufficiently low transparent junctions, where ZBCP clearly splits for d-wave. This unique property originates from the fact that for p-wave superconductors, perpendicularly injected quasiparticles form ZES, which contribute most dominantly to the tunneling conductance. In addition, we show that for p(x) + ip(y)-wave superconductor junctions, the height of ZBCP is sensitive to H due to the formation of a broken time reversal symmetry state. We propose that tunneling spectroscopy in the presence of a magnetic field, i.e., magnetotunneling, is a promising method of determining the pairing symmetry of unconventional superconductors.
引用
收藏
页码:2102 / 2105
页数:4
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