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Features of Chirality Generated by Paramagnetic Coupling to Magnetic Fields in the 3 K-Phase of Sr2RuO4
https://repo.qst.go.jp/records/79636
https://repo.qst.go.jp/records/79636d003ebed-b804-4e85-83a3-ba9d8cb4ebae
| Item type | 会議発表論文 / Conference Paper(1) | |||||
|---|---|---|---|---|---|---|
| 公開日 | 2020-03-25 | |||||
| タイトル | ||||||
| タイトル | Features of Chirality Generated by Paramagnetic Coupling to Magnetic Fields in the 3 K-Phase of Sr2RuO4 | |||||
| 言語 | ||||||
| 言語 | eng | |||||
| 資源タイプ | ||||||
| 資源タイプ識別子 | http://purl.org/coar/resource_type/c_5794 | |||||
| 資源タイプ | conference paper | |||||
| アクセス権 | ||||||
| アクセス権 | metadata only access | |||||
| アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
| 著者 |
Kaneyasu, Hirono
× Kaneyasu, Hirono× Enokida, Yuya× Nomura, Takuji× Hasegawa, Yasumasa× Sakai, Toru× Sigrist, Manfred× Nomura, Takuji× Sakai, Toru |
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| 抄録 | ||||||
| 内容記述タイプ | Abstract | |||||
| 内容記述 | Eutectic Sr2RuO4-Ru samples show an onset of inhomogeneous superconductivity at around 3 K, which is above the bulk transition of Sr2RuO4 (SRO) with Tc≈1.5Tc≈1.5 K. This superconducting state nucleates most likely as a filamentary state at the interface between SRO and Ru- inclusions. Assuming that the superconducting phase of SRO has chiral symmetry, the evolution towards the bulk phase involves an additional symmetry breaking transition. Phenomenological theories based on a two- component order parameter (ηxηx, ηyηy) suggest that first a time reversal symmetry conserving order parameter nucleates at the interface due to the symmetry reduction. A second transition yields a time reversal symmetry breaking phase through the appearance of a second order parameter component. In this study we show how this second transition can be influenced by external magnetic fields. For fields parallel to the basal plane of SRO the transition is suppressed. On the other hand, fields along the c-axis support the second order parameter component. This behavior is well visible in quasi -particle tunneling spectroscopy where a zero-bias peak indicates the presence of the second order parameter component. Our result reproduces experimental results on a qualitative level very well and are compatible with both chiral superconducting phases, px±ipypx±ipy-wave (spin triplet) and dxz±idyzdxz±idyz-wave (spin singlet) pairing. |
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| 書誌情報 |
JPS Conference Proceedings 巻 30, p. 011039-1-011039-6, 発行日 2020-03 |
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| ISSN | ||||||
| 収録物識別子タイプ | ISSN | |||||
| 収録物識別子 | 2435-3892 | |||||
| DOI | ||||||
| 識別子タイプ | DOI | |||||
| 関連識別子 | 10.7566/JPSCP.30.011039 | |||||
| 関連サイト | ||||||
| 識別子タイプ | URI | |||||
| 関連識別子 | https://journals.jps.jp/doi/abs/10.7566/JPSCP.30.011039 | |||||
