A. Alshemi, E. M. Forgan, A. Hiess, R. Cubitt, J. S. White, K. Schmalzl, E. Blackburn
{"title":"对2H−NbSe2超导态的两个特征贡献","authors":"A. Alshemi, E. M. Forgan, A. Hiess, R. Cubitt, J. S. White, K. Schmalzl, E. Blackburn","doi":"10.1103/physrevlett.134.116001","DOIUrl":null,"url":null,"abstract":"Multiband superconductivity arises when multiple electronic bands contribute to the formation of the superconducting state, allowing distinct pairing interactions and gap structures. Here, we present field- and temperature-dependent data on the vortex lattice structure in 2</a:mn>H</a:mi>−</a:mtext>NbSe</a:mtext></a:mrow>2</a:mn></a:mrow></a:msub></a:mrow></a:math> as a contribution to the ongoing debate as to whether the defining feature of the superconductivity is the anisotropy or the multiband nature. The field-dependent data clearly show that there are two distinct superconducting bands, and the contribution of one of them to the vortex lattice signal is completely suppressed for magnetic fields above <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mo>∼</c:mo><c:mn>0.8</c:mn><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi mathvariant=\"normal\">T</c:mi></c:math>, well below <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:msub><f:mrow><f:mi>B</f:mi></f:mrow><f:mrow><f:mi mathvariant=\"normal\">c</f:mi><f:mn>2</f:mn></f:mrow></f:msub></f:math>. By combining the temperature and field scans, we can deduce that there is a moderate degree of interband coupling. From the observed temperature dependences, we find that at low field and zero temperature, the two gaps in temperature units are <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mn>13.1</i:mn><i:mo>±</i:mo><i:mn>0.2</i:mn></i:math> and <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mn>6.5</k:mn><k:mo>±</k:mo><k:mn>0.3</k:mn><k:mtext> </k:mtext><k:mtext> </k:mtext><k:mi mathvariant=\"normal\">K</k:mi></k:math> (<n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><n:msub><n:mi mathvariant=\"normal\">Δ</n:mi><n:mn>0</n:mn></n:msub><n:mo>=</n:mo><n:mn>1.88</n:mn></n:math> and 0.94 <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mrow><q:msub><q:mrow><q:mi>k</q:mi></q:mrow><q:mrow><q:mi mathvariant=\"normal\">B</q:mi></q:mrow></q:msub><q:msub><q:mrow><q:mi>T</q:mi></q:mrow><q:mrow><q:mi mathvariant=\"normal\">c</q:mi></q:mrow></q:msub></q:mrow></q:math>); the band with the larger gap gives just under two-thirds of the superfluid density. The penetration depth extrapolated to zero field and zero temperature is <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mn>160</u:mn><u:mo>±</u:mo><u:mn>2</u:mn><u:mtext> </u:mtext><u:mtext> </u:mtext><u:mi>nm</u:mi></u:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"24 1","pages":""},"PeriodicalIF":9.4000,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Two Characteristic Contributions to the Superconducting State of 2H−NbSe2\",\"authors\":\"A. Alshemi, E. M. Forgan, A. Hiess, R. Cubitt, J. S. White, K. Schmalzl, E. Blackburn\",\"doi\":\"10.1103/physrevlett.134.116001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Multiband superconductivity arises when multiple electronic bands contribute to the formation of the superconducting state, allowing distinct pairing interactions and gap structures. Here, we present field- and temperature-dependent data on the vortex lattice structure in 2</a:mn>H</a:mi>−</a:mtext>NbSe</a:mtext></a:mrow>2</a:mn></a:mrow></a:msub></a:mrow></a:math> as a contribution to the ongoing debate as to whether the defining feature of the superconductivity is the anisotropy or the multiband nature. The field-dependent data clearly show that there are two distinct superconducting bands, and the contribution of one of them to the vortex lattice signal is completely suppressed for magnetic fields above <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mo>∼</c:mo><c:mn>0.8</c:mn><c:mtext> </c:mtext><c:mtext> </c:mtext><c:mi mathvariant=\\\"normal\\\">T</c:mi></c:math>, well below <f:math xmlns:f=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><f:msub><f:mrow><f:mi>B</f:mi></f:mrow><f:mrow><f:mi mathvariant=\\\"normal\\\">c</f:mi><f:mn>2</f:mn></f:mrow></f:msub></f:math>. By combining the temperature and field scans, we can deduce that there is a moderate degree of interband coupling. From the observed temperature dependences, we find that at low field and zero temperature, the two gaps in temperature units are <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:mn>13.1</i:mn><i:mo>±</i:mo><i:mn>0.2</i:mn></i:math> and <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mn>6.5</k:mn><k:mo>±</k:mo><k:mn>0.3</k:mn><k:mtext> </k:mtext><k:mtext> </k:mtext><k:mi mathvariant=\\\"normal\\\">K</k:mi></k:math> (<n:math xmlns:n=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><n:msub><n:mi mathvariant=\\\"normal\\\">Δ</n:mi><n:mn>0</n:mn></n:msub><n:mo>=</n:mo><n:mn>1.88</n:mn></n:math> and 0.94 <q:math xmlns:q=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><q:mrow><q:msub><q:mrow><q:mi>k</q:mi></q:mrow><q:mrow><q:mi mathvariant=\\\"normal\\\">B</q:mi></q:mrow></q:msub><q:msub><q:mrow><q:mi>T</q:mi></q:mrow><q:mrow><q:mi mathvariant=\\\"normal\\\">c</q:mi></q:mrow></q:msub></q:mrow></q:math>); the band with the larger gap gives just under two-thirds of the superfluid density. The penetration depth extrapolated to zero field and zero temperature is <u:math xmlns:u=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><u:mn>160</u:mn><u:mo>±</u:mo><u:mn>2</u:mn><u:mtext> </u:mtext><u:mtext> </u:mtext><u:mi>nm</u:mi></u:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20069,\"journal\":{\"name\":\"Physical review letters\",\"volume\":\"24 1\",\"pages\":\"\"},\"PeriodicalIF\":9.4000,\"publicationDate\":\"2025-03-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical review letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevlett.134.116001\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.134.116001","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
当多个电子带有助于超导态的形成时,就会出现多带超导性,允许不同的配对相互作用和间隙结构。在这里,我们提供了2H−NbSe2中涡晶格结构的场和温度相关数据,作为对超导性的定义特征是各向异性还是多带性质的持续争论的贡献。场相关数据清楚地表明存在两个不同的超导带,其中一个对涡旋晶格信号的贡献在高于~ 0.8 T的磁场中完全被抑制,远低于Bc2。通过结合温度和场扫描,我们可以推断出存在中等程度的带间耦合。从观测到的温度依赖性来看,在低场和零温度下,两个温度单位的差距分别为13.1±0.2和6.5±0.3 K (Δ0=1.88和0.94 kBTc);间隙较大的带的超流体密度略低于三分之二。外推到零场和零温度的穿透深度为160±2 nm。2025年由美国物理学会出版
Two Characteristic Contributions to the Superconducting State of 2H−NbSe2
Multiband superconductivity arises when multiple electronic bands contribute to the formation of the superconducting state, allowing distinct pairing interactions and gap structures. Here, we present field- and temperature-dependent data on the vortex lattice structure in 2H−NbSe2 as a contribution to the ongoing debate as to whether the defining feature of the superconductivity is the anisotropy or the multiband nature. The field-dependent data clearly show that there are two distinct superconducting bands, and the contribution of one of them to the vortex lattice signal is completely suppressed for magnetic fields above ∼0.8T, well below Bc2. By combining the temperature and field scans, we can deduce that there is a moderate degree of interband coupling. From the observed temperature dependences, we find that at low field and zero temperature, the two gaps in temperature units are 13.1±0.2 and 6.5±0.3K (Δ0=1.88 and 0.94 kBTc); the band with the larger gap gives just under two-thirds of the superfluid density. The penetration depth extrapolated to zero field and zero temperature is 160±2nm. Published by the American Physical Society2025
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