Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition
The existence of a nematic phase transition in iron-chalcogenide superconductors poses an intriguing question about its impact on superconductivity. To understand the nature of this unique quantum phase transition, it is essential to study how the electronic structure changes across this transition...
Main Authors: | , , , , , , , , , , , , , , , |
---|---|
Format: | Journal article |
Language: | English |
Published: |
Springer Nature
2019
|
_version_ | 1826307282248400896 |
---|---|
author | Coldea, AI Blake, SF Kasahara, S Haghighirad, AA Watson, MD Knafo, W Choi, ES McCollam, A Reiss, P Yamashita, T Bruma, M Speller, SC Matsuda, Y Wolf, T Shibauchi, T Schofield, AJ |
author_facet | Coldea, AI Blake, SF Kasahara, S Haghighirad, AA Watson, MD Knafo, W Choi, ES McCollam, A Reiss, P Yamashita, T Bruma, M Speller, SC Matsuda, Y Wolf, T Shibauchi, T Schofield, AJ |
author_sort | Coldea, AI |
collection | OXFORD |
description | The existence of a nematic phase transition in iron-chalcogenide superconductors poses an intriguing question about its impact on superconductivity. To understand the nature of this unique quantum phase transition, it is essential to study how the electronic structure changes across this transition at low temperatures. Here, we investigate the evolution of the Fermi surfaces and electronic interactions across the nematic phase transition of FeSe1−xSx using Shubnikov-de Haas oscillations in high magnetic fields up to 45 T in the low temperature regime down to 0.4 K. Most of the Fermi surfaces of FeSe1−xSx monotonically increase in size except for a prominent low frequency oscillation associated with a small, but highly mobile band, which disappears at the nematic phase boundary near x ~ 0.17, indicative of a topological Lifshitz transition. The quasiparticle masses are larger inside the nematic phase, indicative of a strongly correlated state, but they become suppressed outside it. The experimentally observed changes in the Fermi surface topology, together with the varying degree of electronic correlations, will change the balance of electronic interactions in the multi-band system FeSe1−xSx and promote different kz-dependent superconducting pairing channels inside and outside the nematic phase. |
first_indexed | 2024-03-07T07:00:34Z |
format | Journal article |
id | oxford-uuid:ff9b1e9c-29f9-4662-ab2a-688ef27b3718 |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-07T07:00:34Z |
publishDate | 2019 |
publisher | Springer Nature |
record_format | dspace |
spelling | oxford-uuid:ff9b1e9c-29f9-4662-ab2a-688ef27b37182022-03-27T13:46:16ZEvolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transitionJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:ff9b1e9c-29f9-4662-ab2a-688ef27b3718EnglishSymplectic Elements at OxfordSpringer Nature2019Coldea, AIBlake, SFKasahara, SHaghighirad, AAWatson, MDKnafo, WChoi, ESMcCollam, AReiss, PYamashita, TBruma, MSpeller, SCMatsuda, YWolf, TShibauchi, TSchofield, AJThe existence of a nematic phase transition in iron-chalcogenide superconductors poses an intriguing question about its impact on superconductivity. To understand the nature of this unique quantum phase transition, it is essential to study how the electronic structure changes across this transition at low temperatures. Here, we investigate the evolution of the Fermi surfaces and electronic interactions across the nematic phase transition of FeSe1−xSx using Shubnikov-de Haas oscillations in high magnetic fields up to 45 T in the low temperature regime down to 0.4 K. Most of the Fermi surfaces of FeSe1−xSx monotonically increase in size except for a prominent low frequency oscillation associated with a small, but highly mobile band, which disappears at the nematic phase boundary near x ~ 0.17, indicative of a topological Lifshitz transition. The quasiparticle masses are larger inside the nematic phase, indicative of a strongly correlated state, but they become suppressed outside it. The experimentally observed changes in the Fermi surface topology, together with the varying degree of electronic correlations, will change the balance of electronic interactions in the multi-band system FeSe1−xSx and promote different kz-dependent superconducting pairing channels inside and outside the nematic phase. |
spellingShingle | Coldea, AI Blake, SF Kasahara, S Haghighirad, AA Watson, MD Knafo, W Choi, ES McCollam, A Reiss, P Yamashita, T Bruma, M Speller, SC Matsuda, Y Wolf, T Shibauchi, T Schofield, AJ Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title | Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title_full | Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title_fullStr | Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title_full_unstemmed | Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title_short | Evolution of the low-temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition |
title_sort | evolution of the low temperature fermi surface of superconducting fese1 xsx across a nematic phase transition |
work_keys_str_mv | AT coldeaai evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT blakesf evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT kasaharas evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT haghighiradaa evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT watsonmd evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT knafow evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT choies evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT mccollama evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT reissp evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT yamashitat evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT brumam evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT spellersc evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT matsuday evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT wolft evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT shibauchit evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition AT schofieldaj evolutionofthelowtemperaturefermisurfaceofsuperconductingfese1xsxacrossanematicphasetransition |