Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3

When an order parameter has multiple components, fluctuations can suppress the ordering partially, leaving behind vestigial order. Here the authors show that nematic superconductivity in electron-doped Bi2Se3 gives way to a vestigial nematic phase driven by fluctuating Cooper pairs.

Guardado en:
Detalles Bibliográficos
Autores principales: Chang-woo Cho, Junying Shen, Jian Lyu, Omargeldi Atanov, Qianxue Chen, Seng Huat Lee, Yew San Hor, Dariusz Jakub Gawryluk, Ekaterina Pomjakushina, Marek Bartkowiak, Matthias Hecker, Jörg Schmalian, Rolf Lortz
Formato: article
Lenguaje:EN
Publicado: Nature Portfolio 2020
Materias:
Q
Acceso en línea:https://doaj.org/article/14bf7303d1d84fbd938b6acebe6c2ba1
Etiquetas: Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
id oai:doaj.org-article:14bf7303d1d84fbd938b6acebe6c2ba1
record_format dspace
spelling oai:doaj.org-article:14bf7303d1d84fbd938b6acebe6c2ba12021-12-02T17:23:25ZZ 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se310.1038/s41467-020-16871-92041-1723https://doaj.org/article/14bf7303d1d84fbd938b6acebe6c2ba12020-06-01T00:00:00Zhttps://doi.org/10.1038/s41467-020-16871-9https://doaj.org/toc/2041-1723When an order parameter has multiple components, fluctuations can suppress the ordering partially, leaving behind vestigial order. Here the authors show that nematic superconductivity in electron-doped Bi2Se3 gives way to a vestigial nematic phase driven by fluctuating Cooper pairs.Chang-woo ChoJunying ShenJian LyuOmargeldi AtanovQianxue ChenSeng Huat LeeYew San HorDariusz Jakub GawrylukEkaterina PomjakushinaMarek BartkowiakMatthias HeckerJörg SchmalianRolf LortzNature PortfolioarticleScienceQENNature Communications, Vol 11, Iss 1, Pp 1-8 (2020)
institution DOAJ
collection DOAJ
language EN
topic Science
Q
spellingShingle Science
Q
Chang-woo Cho
Junying Shen
Jian Lyu
Omargeldi Atanov
Qianxue Chen
Seng Huat Lee
Yew San Hor
Dariusz Jakub Gawryluk
Ekaterina Pomjakushina
Marek Bartkowiak
Matthias Hecker
Jörg Schmalian
Rolf Lortz
Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
description When an order parameter has multiple components, fluctuations can suppress the ordering partially, leaving behind vestigial order. Here the authors show that nematic superconductivity in electron-doped Bi2Se3 gives way to a vestigial nematic phase driven by fluctuating Cooper pairs.
format article
author Chang-woo Cho
Junying Shen
Jian Lyu
Omargeldi Atanov
Qianxue Chen
Seng Huat Lee
Yew San Hor
Dariusz Jakub Gawryluk
Ekaterina Pomjakushina
Marek Bartkowiak
Matthias Hecker
Jörg Schmalian
Rolf Lortz
author_facet Chang-woo Cho
Junying Shen
Jian Lyu
Omargeldi Atanov
Qianxue Chen
Seng Huat Lee
Yew San Hor
Dariusz Jakub Gawryluk
Ekaterina Pomjakushina
Marek Bartkowiak
Matthias Hecker
Jörg Schmalian
Rolf Lortz
author_sort Chang-woo Cho
title Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
title_short Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
title_full Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
title_fullStr Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
title_full_unstemmed Z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators NbxBi2Se3 and CuxBi2Se3
title_sort z 3-vestigial nematic order due to superconducting fluctuations in the doped topological insulators nbxbi2se3 and cuxbi2se3
publisher Nature Portfolio
publishDate 2020
url https://doaj.org/article/14bf7303d1d84fbd938b6acebe6c2ba1
work_keys_str_mv AT changwoocho z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT junyingshen z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT jianlyu z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT omargeldiatanov z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT qianxuechen z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT senghuatlee z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT yewsanhor z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT dariuszjakubgawryluk z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT ekaterinapomjakushina z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT marekbartkowiak z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT matthiashecker z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT jorgschmalian z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
AT rolflortz z3vestigialnematicorderduetosuperconductingfluctuationsinthedopedtopologicalinsulatorsnbxbi2se3andcuxbi2se3
_version_ 1718380953327370240