Superconducting Gap Anisotropy in Monolayer FeSe Thin Film
Superconductivity originates from pairing of electrons near the Fermi energy. The Fermi surface topology and pairing symmetry are thus two pivotal characteristics of a superconductor. Superconductivity in one monolayer (1 ML) FeSe thin film has attracted great interest recently due to its intriguing...
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Veröffentlicht in: | Physical review letters 2016-09, Vol.117 (11), p.117001-117001, Article 117001 |
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creator | Zhang, Y Lee, J J Moore, R G Li, W Yi, M Hashimoto, M Lu, D H Devereaux, T P Lee, D-H Shen, Z-X |
description | Superconductivity originates from pairing of electrons near the Fermi energy. The Fermi surface topology and pairing symmetry are thus two pivotal characteristics of a superconductor. Superconductivity in one monolayer (1 ML) FeSe thin film has attracted great interest recently due to its intriguing interfacial properties and possibly high superconducting transition temperature over 65 K. Here, we report high-resolution measurements of the Fermi surface and superconducting gaps in 1 ML FeSe using angle-resolved photoemission spectroscopy. Two ellipselike electron pockets are clearly resolved overlapping with each other at the Brillouin zone corner. The superconducting gap is nodeless but moderately anisotropic, which puts strong constraint on determining the pairing symmetry. The gap maxima locate on the d_{xy} bands along the major axis of the ellipse and four gap minima are observed at the intersections of electron pockets. The gap maximum location combined with the Fermi surface geometry deviate from a single d-wave, extended s-wave or s_{±} gap function, suggesting an important role of the multiorbital nature of Fermi surface and orbital-dependent pairing in 1 ML FeSe. The gap minima location may be explained by a sign change on the electron pockets, or a competition between intra- and interorbital pairing. |
doi_str_mv | 10.1103/PhysRevLett.117.117001 |
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The Fermi surface topology and pairing symmetry are thus two pivotal characteristics of a superconductor. Superconductivity in one monolayer (1 ML) FeSe thin film has attracted great interest recently due to its intriguing interfacial properties and possibly high superconducting transition temperature over 65 K. Here, we report high-resolution measurements of the Fermi surface and superconducting gaps in 1 ML FeSe using angle-resolved photoemission spectroscopy. Two ellipselike electron pockets are clearly resolved overlapping with each other at the Brillouin zone corner. The superconducting gap is nodeless but moderately anisotropic, which puts strong constraint on determining the pairing symmetry. The gap maxima locate on the d_{xy} bands along the major axis of the ellipse and four gap minima are observed at the intersections of electron pockets. The gap maximum location combined with the Fermi surface geometry deviate from a single d-wave, extended s-wave or s_{±} gap function, suggesting an important role of the multiorbital nature of Fermi surface and orbital-dependent pairing in 1 ML FeSe. The gap minima location may be explained by a sign change on the electron pockets, or a competition between intra- and interorbital pairing.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.117.117001</identifier><identifier>PMID: 27661715</identifier><language>eng</language><publisher>United States</publisher><subject>Anisotropy ; Fermi surfaces ; Minima ; Monolayers ; Pocket ; Superconductivity ; Symmetry ; Thin films</subject><ispartof>Physical review letters, 2016-09, Vol.117 (11), p.117001-117001, Article 117001</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c410t-f388d818bd81a478c1488af9cad120bb712bc70eeb7b496ec877c6f2982481633</citedby><cites>FETCH-LOGICAL-c410t-f388d818bd81a478c1488af9cad120bb712bc70eeb7b496ec877c6f2982481633</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,2863,2864,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27661715$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Zhang, Y</creatorcontrib><creatorcontrib>Lee, J J</creatorcontrib><creatorcontrib>Moore, R G</creatorcontrib><creatorcontrib>Li, W</creatorcontrib><creatorcontrib>Yi, M</creatorcontrib><creatorcontrib>Hashimoto, M</creatorcontrib><creatorcontrib>Lu, D H</creatorcontrib><creatorcontrib>Devereaux, T P</creatorcontrib><creatorcontrib>Lee, D-H</creatorcontrib><creatorcontrib>Shen, Z-X</creatorcontrib><title>Superconducting Gap Anisotropy in Monolayer FeSe Thin Film</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>Superconductivity originates from pairing of electrons near the Fermi energy. The Fermi surface topology and pairing symmetry are thus two pivotal characteristics of a superconductor. Superconductivity in one monolayer (1 ML) FeSe thin film has attracted great interest recently due to its intriguing interfacial properties and possibly high superconducting transition temperature over 65 K. Here, we report high-resolution measurements of the Fermi surface and superconducting gaps in 1 ML FeSe using angle-resolved photoemission spectroscopy. Two ellipselike electron pockets are clearly resolved overlapping with each other at the Brillouin zone corner. The superconducting gap is nodeless but moderately anisotropic, which puts strong constraint on determining the pairing symmetry. The gap maxima locate on the d_{xy} bands along the major axis of the ellipse and four gap minima are observed at the intersections of electron pockets. The gap maximum location combined with the Fermi surface geometry deviate from a single d-wave, extended s-wave or s_{±} gap function, suggesting an important role of the multiorbital nature of Fermi surface and orbital-dependent pairing in 1 ML FeSe. The gap minima location may be explained by a sign change on the electron pockets, or a competition between intra- and interorbital pairing.</description><subject>Anisotropy</subject><subject>Fermi surfaces</subject><subject>Minima</subject><subject>Monolayers</subject><subject>Pocket</subject><subject>Superconductivity</subject><subject>Symmetry</subject><subject>Thin films</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqNkFFLwzAUhYMobk7_wuijL9XcJEtS38ZwU5gobj6XNE1dpW1q0gr992Zsio8-3Hvh8J1z4SA0BXwDgOnty27wr-ZrbbouCGI_GMMJGgMWSSwA2CkaY0whTjAWI3Th_QcOBOHyHI2I4BwEzMbobtO3xmnb5L3uyuY9Wqk2mjelt52z7RCVTfRkG1upwbhoaTYm2u6Ctiyr-hKdFary5up4J-hteb9dPMTr59XjYr6ONQPcxQWVMpcgs7AUE1IDk1IViVY5EJxlAkimBTYmExlLuNFSCM0LkkjCJHBKJ-j6kNs6-9kb36V16bWpKtUY2_sUJJuFfEbxP1ASKEEYDyg_oNpZ750p0taVtXJDCjjdV5z-qTgIIj1UHIzT448-q03-a_vplH4DxRB42w</recordid><startdate>20160909</startdate><enddate>20160909</enddate><creator>Zhang, Y</creator><creator>Lee, J J</creator><creator>Moore, R G</creator><creator>Li, W</creator><creator>Yi, M</creator><creator>Hashimoto, M</creator><creator>Lu, D H</creator><creator>Devereaux, T P</creator><creator>Lee, D-H</creator><creator>Shen, Z-X</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20160909</creationdate><title>Superconducting Gap Anisotropy in Monolayer FeSe Thin Film</title><author>Zhang, Y ; Lee, J J ; Moore, R G ; Li, W ; Yi, M ; Hashimoto, M ; Lu, D H ; Devereaux, T P ; Lee, D-H ; Shen, Z-X</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c410t-f388d818bd81a478c1488af9cad120bb712bc70eeb7b496ec877c6f2982481633</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Anisotropy</topic><topic>Fermi surfaces</topic><topic>Minima</topic><topic>Monolayers</topic><topic>Pocket</topic><topic>Superconductivity</topic><topic>Symmetry</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhang, Y</creatorcontrib><creatorcontrib>Lee, J J</creatorcontrib><creatorcontrib>Moore, R G</creatorcontrib><creatorcontrib>Li, W</creatorcontrib><creatorcontrib>Yi, M</creatorcontrib><creatorcontrib>Hashimoto, M</creatorcontrib><creatorcontrib>Lu, D H</creatorcontrib><creatorcontrib>Devereaux, T P</creatorcontrib><creatorcontrib>Lee, D-H</creatorcontrib><creatorcontrib>Shen, Z-X</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhang, Y</au><au>Lee, J J</au><au>Moore, R G</au><au>Li, W</au><au>Yi, M</au><au>Hashimoto, M</au><au>Lu, D H</au><au>Devereaux, T P</au><au>Lee, D-H</au><au>Shen, Z-X</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Superconducting Gap Anisotropy in Monolayer FeSe Thin Film</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2016-09-09</date><risdate>2016</risdate><volume>117</volume><issue>11</issue><spage>117001</spage><epage>117001</epage><pages>117001-117001</pages><artnum>117001</artnum><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>Superconductivity originates from pairing of electrons near the Fermi energy. The Fermi surface topology and pairing symmetry are thus two pivotal characteristics of a superconductor. Superconductivity in one monolayer (1 ML) FeSe thin film has attracted great interest recently due to its intriguing interfacial properties and possibly high superconducting transition temperature over 65 K. Here, we report high-resolution measurements of the Fermi surface and superconducting gaps in 1 ML FeSe using angle-resolved photoemission spectroscopy. Two ellipselike electron pockets are clearly resolved overlapping with each other at the Brillouin zone corner. The superconducting gap is nodeless but moderately anisotropic, which puts strong constraint on determining the pairing symmetry. The gap maxima locate on the d_{xy} bands along the major axis of the ellipse and four gap minima are observed at the intersections of electron pockets. The gap maximum location combined with the Fermi surface geometry deviate from a single d-wave, extended s-wave or s_{±} gap function, suggesting an important role of the multiorbital nature of Fermi surface and orbital-dependent pairing in 1 ML FeSe. The gap minima location may be explained by a sign change on the electron pockets, or a competition between intra- and interorbital pairing.</abstract><cop>United States</cop><pmid>27661715</pmid><doi>10.1103/PhysRevLett.117.117001</doi><tpages>1</tpages></addata></record> |
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subjects | Anisotropy Fermi surfaces Minima Monolayers Superconductivity Symmetry Thin films |
title | Superconducting Gap Anisotropy in Monolayer FeSe Thin Film |
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