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Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)

The quantum vortex liquid (QVL) is an intriguing state of type-II superconductors in which intense quantum fluctuations of the superconducting (SC) order parameter destroy the Abrikosov lattice even at very low temperatures. Such a state has only rarely been observed, however, and remains poorly und...

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Autores principales: Čulo, M., Licciardello, S., Ishida, K., Mukasa, K., Ayres, J., Buhot, J., Hsu, Y.-T., Imajo, S., Qiu, M. W., Saito, M., Uezono, Y., Otsuka, T., Watanabe, T., Kindo, K., Shibauchi, T., Kasahara, S., Matsuda, Y., Hussey, N. E.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10338513/
https://www.ncbi.nlm.nih.gov/pubmed/37438333
http://dx.doi.org/10.1038/s41467-023-39730-9
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author Čulo, M.
Licciardello, S.
Ishida, K.
Mukasa, K.
Ayres, J.
Buhot, J.
Hsu, Y.-T.
Imajo, S.
Qiu, M. W.
Saito, M.
Uezono, Y.
Otsuka, T.
Watanabe, T.
Kindo, K.
Shibauchi, T.
Kasahara, S.
Matsuda, Y.
Hussey, N. E.
author_facet Čulo, M.
Licciardello, S.
Ishida, K.
Mukasa, K.
Ayres, J.
Buhot, J.
Hsu, Y.-T.
Imajo, S.
Qiu, M. W.
Saito, M.
Uezono, Y.
Otsuka, T.
Watanabe, T.
Kindo, K.
Shibauchi, T.
Kasahara, S.
Matsuda, Y.
Hussey, N. E.
author_sort Čulo, M.
collection PubMed
description The quantum vortex liquid (QVL) is an intriguing state of type-II superconductors in which intense quantum fluctuations of the superconducting (SC) order parameter destroy the Abrikosov lattice even at very low temperatures. Such a state has only rarely been observed, however, and remains poorly understood. One of the key questions is the precise origin of such intense quantum fluctuations and the role of nearby non-SC phases or quantum critical points in amplifying these effects. Here we report a high-field magnetotransport study of FeSe(1−x)S(x) and FeSe(1−x)Te(x) which show a broad QVL regime both within and beyond their respective electron nematic phases. A clear correlation is found between the extent of the QVL and the strength of the superconductivity. This comparative study enables us to identify the essential elements that promote the QVL regime in unconventional superconductors and to demonstrate that the QVL regime itself is most extended wherever superconductivity is weakest.
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spelling pubmed-103385132023-07-14 Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x) Čulo, M. Licciardello, S. Ishida, K. Mukasa, K. Ayres, J. Buhot, J. Hsu, Y.-T. Imajo, S. Qiu, M. W. Saito, M. Uezono, Y. Otsuka, T. Watanabe, T. Kindo, K. Shibauchi, T. Kasahara, S. Matsuda, Y. Hussey, N. E. Nat Commun Article The quantum vortex liquid (QVL) is an intriguing state of type-II superconductors in which intense quantum fluctuations of the superconducting (SC) order parameter destroy the Abrikosov lattice even at very low temperatures. Such a state has only rarely been observed, however, and remains poorly understood. One of the key questions is the precise origin of such intense quantum fluctuations and the role of nearby non-SC phases or quantum critical points in amplifying these effects. Here we report a high-field magnetotransport study of FeSe(1−x)S(x) and FeSe(1−x)Te(x) which show a broad QVL regime both within and beyond their respective electron nematic phases. A clear correlation is found between the extent of the QVL and the strength of the superconductivity. This comparative study enables us to identify the essential elements that promote the QVL regime in unconventional superconductors and to demonstrate that the QVL regime itself is most extended wherever superconductivity is weakest. Nature Publishing Group UK 2023-07-12 /pmc/articles/PMC10338513/ /pubmed/37438333 http://dx.doi.org/10.1038/s41467-023-39730-9 Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Čulo, M.
Licciardello, S.
Ishida, K.
Mukasa, K.
Ayres, J.
Buhot, J.
Hsu, Y.-T.
Imajo, S.
Qiu, M. W.
Saito, M.
Uezono, Y.
Otsuka, T.
Watanabe, T.
Kindo, K.
Shibauchi, T.
Kasahara, S.
Matsuda, Y.
Hussey, N. E.
Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title_full Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title_fullStr Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title_full_unstemmed Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title_short Expanded quantum vortex liquid regimes in the electron nematic superconductors FeSe(1−x)S(x) and FeSe(1−x)Te(x)
title_sort expanded quantum vortex liquid regimes in the electron nematic superconductors fese(1−x)s(x) and fese(1−x)te(x)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10338513/
https://www.ncbi.nlm.nih.gov/pubmed/37438333
http://dx.doi.org/10.1038/s41467-023-39730-9
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