顺磁去耦诱导的d波超导与反铁磁共存
超导电性
2015-05-19 v2
摘要
理论上证明,在具有配对的超导态中,强泡利顺磁去耦(PD)不仅会诱导调制的Fulde-Ferrell-Larkin-Ovchinnikov (FFLO)超导态,还会诱导出矢量几乎平行于能隙节点的非公度反铁磁(AFM)(或自旋密度波)有序。这种场诱导的d波超导与AFM序共存的固有机制无需假设对密度波,而是由FFLO有序增强的。论证表明,这既是CeCoIn中共存FFLO和AFM相的共同起源,也是在几种重费米子超导体和过掺杂铜氧化物中观察到的超导附近AFM量子临界行为的共同起源。
引用
@article{arxiv.1006.2465,
title = {Coexistence of d-wave superconductivity and antiferromagnetism induced by paramagnetic depairing},
author = {Yuhki Hatakeyama and Ryusuke Ikeda},
journal= {arXiv preprint arXiv:1006.2465},
year = {2015}
}
备注
4 pages, 2 figures, the version accepted for publication in J.Phys.Conf.Series (Proc. of SCES2010)