{"title":"通过双束脉冲激光沉积探究 FeSe 薄膜中 T c 变化大的原因。","authors":"Zhongpei Feng, Hua Zhang, Jie Yuan, Xingyu Jiang, Xianxin Wu, Zhanyi Zhao, Qiuhao Xu, Valentin Stanev, Qinghua Zhang, Huaixin Yang, Lin Gu, Sheng Meng, Suming Weng, Qihong Chen, Ichiro Takeuchi, Kui Jin, Zhongxian Zhao","doi":"10.1007/s44214-024-00058-0","DOIUrl":null,"url":null,"abstract":"<p><p>FeSe is one of the most enigmatic superconductors. Among the family of iron-based compounds, it has the simplest chemical makeup and structure, and yet it displays superconducting transition temperature ( <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> ) spanning 0 to 15 K for thin films, while it is typically 8 K for single crystals. This large variation of <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> within one family underscores a key challenge associated with understanding superconductivity in iron chalcogenides. Here, using a dual-beam pulsed laser deposition (PLD) approach, we have fabricated a unique lattice-constant gradient thin film of FeSe which has revealed a clear relationship between the atomic structure and the superconducting transition temperature for the first time. The dual-beam PLD that generates laser fluence gradient inside the plasma plume has resulted in a continuous variation in distribution of edge dislocations within a single film, and a precise correlation between the lattice constant and <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> has been observed here, namely, <math><msub><mi>T</mi> <mtext>c</mtext></msub> <mo>∝</mo> <msqrt><mrow><mi>c</mi> <mo>-</mo> <msub><mi>c</mi> <mn>0</mn></msub> </mrow> </msqrt> </math> , where <i>c</i> is the <i>c</i>-axis lattice constant (and <math><msub><mi>c</mi> <mn>0</mn></msub> </math> is a constant). This explicit relation in conjunction with a theoretical investigation indicates that it is the shifting of the <math><msub><mi>d</mi> <mtext>xy</mtext></msub> </math> orbital of Fe which plays a governing role in the interplay between nematicity and superconductivity in FeSe.</p><p><strong>Supplementary information: </strong>The online version contains supplementary material available at 10.1007/s44214-024-00058-0.</p>","PeriodicalId":74629,"journal":{"name":"Quantum frontiers","volume":"3 1","pages":"12"},"PeriodicalIF":0.0000,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11161545/pdf/","citationCount":"0","resultStr":"{\"title\":\"<ArticleTitle xmlns:ns0=\\\"http://www.w3.org/1998/Math/MathML\\\">The origin of the large <ns0:math><ns0:msub><ns0:mi>T</ns0:mi> <ns0:mi>c</ns0:mi></ns0:msub> </ns0:math> variation in FeSe thin films probed by dual-beam pulsed laser deposition.\",\"authors\":\"Zhongpei Feng, Hua Zhang, Jie Yuan, Xingyu Jiang, Xianxin Wu, Zhanyi Zhao, Qiuhao Xu, Valentin Stanev, Qinghua Zhang, Huaixin Yang, Lin Gu, Sheng Meng, Suming Weng, Qihong Chen, Ichiro Takeuchi, Kui Jin, Zhongxian Zhao\",\"doi\":\"10.1007/s44214-024-00058-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>FeSe is one of the most enigmatic superconductors. Among the family of iron-based compounds, it has the simplest chemical makeup and structure, and yet it displays superconducting transition temperature ( <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> ) spanning 0 to 15 K for thin films, while it is typically 8 K for single crystals. This large variation of <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> within one family underscores a key challenge associated with understanding superconductivity in iron chalcogenides. Here, using a dual-beam pulsed laser deposition (PLD) approach, we have fabricated a unique lattice-constant gradient thin film of FeSe which has revealed a clear relationship between the atomic structure and the superconducting transition temperature for the first time. The dual-beam PLD that generates laser fluence gradient inside the plasma plume has resulted in a continuous variation in distribution of edge dislocations within a single film, and a precise correlation between the lattice constant and <math><msub><mi>T</mi> <mtext>c</mtext></msub> </math> has been observed here, namely, <math><msub><mi>T</mi> <mtext>c</mtext></msub> <mo>∝</mo> <msqrt><mrow><mi>c</mi> <mo>-</mo> <msub><mi>c</mi> <mn>0</mn></msub> </mrow> </msqrt> </math> , where <i>c</i> is the <i>c</i>-axis lattice constant (and <math><msub><mi>c</mi> <mn>0</mn></msub> </math> is a constant). This explicit relation in conjunction with a theoretical investigation indicates that it is the shifting of the <math><msub><mi>d</mi> <mtext>xy</mtext></msub> </math> orbital of Fe which plays a governing role in the interplay between nematicity and superconductivity in FeSe.</p><p><strong>Supplementary information: </strong>The online version contains supplementary material available at 10.1007/s44214-024-00058-0.</p>\",\"PeriodicalId\":74629,\"journal\":{\"name\":\"Quantum frontiers\",\"volume\":\"3 1\",\"pages\":\"12\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11161545/pdf/\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Quantum frontiers\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1007/s44214-024-00058-0\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2024/6/8 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Quantum frontiers","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/s44214-024-00058-0","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2024/6/8 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
FeSe 是最神秘的超导体之一。在铁基化合物家族中,它的化学组成和结构最简单,但它的薄膜超导转变温度(T c)却在 0 到 15 K 之间,而单晶体的温度通常为 8 K。一个家族中 T c 的巨大差异凸显了了解铁铬镓化合物超导性的关键挑战。在这里,我们利用双光束脉冲激光沉积(PLD)方法,制造出了一种独特的晶格恒定梯度硒化铁薄膜,首次揭示了原子结构与超导转变温度之间的明确关系。在等离子体羽流内部产生激光通量梯度的双光束 PLD 使单层薄膜内的边缘位错分布发生了连续变化,并在此观察到了晶格常数与 T c 之间的精确相关性,即 T c ∝ c - c 0,其中 c 为 c 轴晶格常数(c 0 为常数)。这种明确的关系与理论研究相结合表明,铁的 d xy 轨道移动在 FeSe 的向列性与超导性之间的相互作用中起着支配作用:在线版本包含补充材料,可查阅 10.1007/s44214-024-00058-0。
The origin of the large Tc variation in FeSe thin films probed by dual-beam pulsed laser deposition.
FeSe is one of the most enigmatic superconductors. Among the family of iron-based compounds, it has the simplest chemical makeup and structure, and yet it displays superconducting transition temperature ( ) spanning 0 to 15 K for thin films, while it is typically 8 K for single crystals. This large variation of within one family underscores a key challenge associated with understanding superconductivity in iron chalcogenides. Here, using a dual-beam pulsed laser deposition (PLD) approach, we have fabricated a unique lattice-constant gradient thin film of FeSe which has revealed a clear relationship between the atomic structure and the superconducting transition temperature for the first time. The dual-beam PLD that generates laser fluence gradient inside the plasma plume has resulted in a continuous variation in distribution of edge dislocations within a single film, and a precise correlation between the lattice constant and has been observed here, namely, , where c is the c-axis lattice constant (and is a constant). This explicit relation in conjunction with a theoretical investigation indicates that it is the shifting of the orbital of Fe which plays a governing role in the interplay between nematicity and superconductivity in FeSe.
Supplementary information: The online version contains supplementary material available at 10.1007/s44214-024-00058-0.