Topological structure of the inter-band phase difference soliton in two-band superconductivity

被引:5
|
作者
Tanaka, Y. [1 ]
Iyo, A. [1 ]
Tokiwa, K. [2 ]
Watanabe, T. [2 ]
Crisan, A. [3 ,4 ]
Sundaresan, A. [5 ]
Terada, N. [6 ]
机构
[1] Natl Inst Adv Ind Sci & Technol, Tsukuba, Ibaraki, Japan
[2] Tokyo Univ Sci, Noda, Chiba 278, Japan
[3] Univ Birmingham, Birmingham, W Midlands, England
[4] Natl Inst Mat Phys, Bucharest, Romania
[5] Indian Inst Sci, Jawaharlal Nehru Ctr Adv Sci Res, Bangalore 560012, Karnataka, India
[6] Kagoshima Univ, Kagoshima 890, Japan
来源
基金
日本科学技术振兴机构;
关键词
i-Soliton; Weinberg-Salam model; Yang-Mills theory; SU(2); UNCONVENTIONAL SUPERCONDUCTOR; VORTEX STRUCTURE; SUPERFLUID HE-3; MODEL; SPIN;
D O I
10.1016/j.physc.2010.05.022
中图分类号
O59 [应用物理学];
学科分类号
摘要
Two-component superconductivity based on the two-band superconductor has a functional topology such as an inter-band phase difference soliton (i-soliton) to realize topological electronics (topolonics). Many gauge field theories are applied to investigate the topology of two-band superconductivity. To ease experimental and electronics applications, these theories should be refined. Weinberg-Salam theory and SU(2) (two-dimensional special unitary symmetry) gauge field theory are proper starting points. An effective extra force field because of the crystal structure and inter-band Josephson interaction, rather than spontaneous symmetry breaking, simplifies the conventional gauge field theory. Crown Copyright (C) 2010 Published by Elsevier B.V. All rights reserved.
引用
收藏
页码:1010 / 1012
页数:3
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