Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4
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 ≈ 1.5 K. This superconducting state nucleates most likely as a filamentary state at the interface between SRO and Ru-inclusions. Assuming that the su...
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ftnirs:oai:repo.qst.go.jp:00078005 2023-05-15T16:55:51+02:00 Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 Kaneyasu Hirono Enokida Yuya Nomura Takuji Hasegawa Yasumasa Sakai Toru Sigrist Manfred 2019-12-16 https://repo.qst.go.jp/?action=repository_uri&item_id=78005 http://id.nii.ac.jp/1657/00077987/ en eng https://repo.qst.go.jp/?action=repository_uri&item_id=78005 http://id.nii.ac.jp/1657/00077987/ 2019-09-25 Presentation 2019 ftnirs 2021-12-30T08:13:05Z 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 ≈ 1.5 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 (ηx, ηy) 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 ±ipy-wave (spin triplet) and dxy ±idyz-wave (spin singlet) pairing. International Conference on Strongly Correlated Electron Systems 2019, SCES ‘19 Conference Object IPY National Institute of Radiological Science: NIRS-Repository |
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National Institute of Radiological Science: NIRS-Repository |
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English |
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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 ≈ 1.5 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 (ηx, ηy) 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 ±ipy-wave (spin triplet) and dxy ±idyz-wave (spin singlet) pairing. International Conference on Strongly Correlated Electron Systems 2019, SCES ‘19 |
format |
Conference Object |
author |
Kaneyasu Hirono Enokida Yuya Nomura Takuji Hasegawa Yasumasa Sakai Toru Sigrist Manfred |
spellingShingle |
Kaneyasu Hirono Enokida Yuya Nomura Takuji Hasegawa Yasumasa Sakai Toru Sigrist Manfred Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
author_facet |
Kaneyasu Hirono Enokida Yuya Nomura Takuji Hasegawa Yasumasa Sakai Toru Sigrist Manfred |
author_sort |
Kaneyasu Hirono |
title |
Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
title_short |
Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
title_full |
Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
title_fullStr |
Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
title_full_unstemmed |
Features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3K-phase of Sr2RuO4 |
title_sort |
features of chirality generated by paramagnetic supercurrents in a magnetic field in the 3k-phase of sr2ruo4 |
publishDate |
2019 |
url |
https://repo.qst.go.jp/?action=repository_uri&item_id=78005 http://id.nii.ac.jp/1657/00077987/ |
genre |
IPY |
genre_facet |
IPY |
op_relation |
https://repo.qst.go.jp/?action=repository_uri&item_id=78005 http://id.nii.ac.jp/1657/00077987/ 2019-09-25 |
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1766046904266784768 |