Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]

The search for unconventional superconductivity has been focused on materials with strong spin-orbit coupling and unique crystal lattices. Doped bismuth selenide (Bi[subscript 2]Se[subscript 3]) is a strong candidate, given the topological insulator nature of the parent compound and its triangular l...

Full description

Bibliographic Details
Main Authors: Asaba, Tomoya, Lawson, B. J., Tinsman, Colin, Chen, Lu, Corbae, Paul, Li, Gang, Qiu, Y., Hor, Y. S., Li, Lu, Fu, Liang
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:English
Published: American Physical Society 2017
Online Access:http://hdl.handle.net/1721.1/107478
https://orcid.org/0000-0002-8803-1017
_version_ 1811072114941231104
author Asaba, Tomoya
Lawson, B. J.
Tinsman, Colin
Chen, Lu
Corbae, Paul
Li, Gang
Qiu, Y.
Hor, Y. S.
Li, Lu
Fu, Liang
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Asaba, Tomoya
Lawson, B. J.
Tinsman, Colin
Chen, Lu
Corbae, Paul
Li, Gang
Qiu, Y.
Hor, Y. S.
Li, Lu
Fu, Liang
author_sort Asaba, Tomoya
collection MIT
description The search for unconventional superconductivity has been focused on materials with strong spin-orbit coupling and unique crystal lattices. Doped bismuth selenide (Bi[subscript 2]Se[subscript 3]) is a strong candidate, given the topological insulator nature of the parent compound and its triangular lattice. The coupling between the physical properties in the superconducting state and its underlying crystal symmetry is a crucial test for unconventional superconductivity. In this paper, we report direct evidence that the superconducting magnetic response couples strongly to the underlying trigonal crystal symmetry in the recently discovered superconductor with trigonal crystal structure, niobium (Nb)-doped Bi[subscript 2]Se[subscript 3]. As a result, the in-plane magnetic torque signal vanishes every 60°. More importantly, the superconducting hysteresis loop amplitude is enhanced along one preferred direction, spontaneously breaking the rotational symmetry. This observation indicates the presence of nematic order in the superconducting ground state of Nb-doped Bi[subscript 2]Se[subscript 3].
first_indexed 2024-09-23T09:01:07Z
format Article
id mit-1721.1/107478
institution Massachusetts Institute of Technology
language English
last_indexed 2024-09-23T09:01:07Z
publishDate 2017
publisher American Physical Society
record_format dspace
spelling mit-1721.1/1074782022-09-26T09:52:14Z Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3] Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi2Se3 Asaba, Tomoya Lawson, B. J. Tinsman, Colin Chen, Lu Corbae, Paul Li, Gang Qiu, Y. Hor, Y. S. Li, Lu Fu, Liang Massachusetts Institute of Technology. Department of Physics Fu, Liang The search for unconventional superconductivity has been focused on materials with strong spin-orbit coupling and unique crystal lattices. Doped bismuth selenide (Bi[subscript 2]Se[subscript 3]) is a strong candidate, given the topological insulator nature of the parent compound and its triangular lattice. The coupling between the physical properties in the superconducting state and its underlying crystal symmetry is a crucial test for unconventional superconductivity. In this paper, we report direct evidence that the superconducting magnetic response couples strongly to the underlying trigonal crystal symmetry in the recently discovered superconductor with trigonal crystal structure, niobium (Nb)-doped Bi[subscript 2]Se[subscript 3]. As a result, the in-plane magnetic torque signal vanishes every 60°. More importantly, the superconducting hysteresis loop amplitude is enhanced along one preferred direction, spontaneously breaking the rotational symmetry. This observation indicates the presence of nematic order in the superconducting ground state of Nb-doped Bi[subscript 2]Se[subscript 3]. United States. Dept. of Energy (Grant DE-SC0008110) National Science Foundation (U.S.) (Grant DMR-1255607) David & Lucile Packard Foundation 2017-03-17T19:20:02Z 2017-03-17T19:20:02Z 2017-01 2016-11 2017-01-27T23:00:02Z Article http://purl.org/eprint/type/JournalArticle 2160-3308 http://hdl.handle.net/1721.1/107478 Asaba, Tomoya et al. “Rotational Symmetry Breaking in a Trigonal Superconductor Nb-Doped Bi 2 Se 3.” Physical Review X 7.1 (2017): n. pag. © 2017 American Physical Society https://orcid.org/0000-0002-8803-1017 en http://dx.doi.org/10.1103/PhysRevX.7.011009 Physical Review X Creative Commons Attribution http://creativecommons.org/licenses/by/3.0 authors application/pdf American Physical Society American Physical Society
spellingShingle Asaba, Tomoya
Lawson, B. J.
Tinsman, Colin
Chen, Lu
Corbae, Paul
Li, Gang
Qiu, Y.
Hor, Y. S.
Li, Lu
Fu, Liang
Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title_full Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title_fullStr Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title_full_unstemmed Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title_short Rotational Symmetry Breaking in a Trigonal Superconductor Nb-doped Bi[subscript 2]Se[subscript 3]
title_sort rotational symmetry breaking in a trigonal superconductor nb doped bi subscript 2 se subscript 3
url http://hdl.handle.net/1721.1/107478
https://orcid.org/0000-0002-8803-1017
work_keys_str_mv AT asabatomoya rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT lawsonbj rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT tinsmancolin rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT chenlu rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT corbaepaul rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT ligang rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT qiuy rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT horys rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT lilu rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT fuliang rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbisubscript2sesubscript3
AT asabatomoya rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT lawsonbj rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT tinsmancolin rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT chenlu rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT corbaepaul rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT ligang rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT qiuy rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT horys rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT lilu rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3
AT fuliang rotationalsymmetrybreakinginatrigonalsuperconductornbdopedbi2se3