{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1362825894045590144.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1063/1.4947433"}},{"identifier":{"@type":"URI","@value":"https://pubs.aip.org/aip/apl/article-pdf/doi/10.1063/1.4947433/13865865/162601_1_online.pdf"}}],"dc:title":[{"@value":"Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Two-dimensional transition-metal dichalcogenide (TMDs) MoTe2 has attracted much attention due to its predicted Weyl semimetal state and a quantum spin Hall insulator in bulk and monolayer form, respectively. We find that the superconductivity in MoTe2 single crystal can be greatly enhanced by the partial substitution of the Te ions by the S ones. The maximum superconducting temperature TC of MoTe1.8S0.2 single crystal is about 1.3 K. Compared with the parent MoTe2 single crystal (TC = 0.1 K), nearly 13-fold in TC is improved in the MoTe1.8S0.2 one. The superconductivity has been investigated through the resistivity and magnetization measurements. MoTe2−xSx single crystals belong to weak coupling superconductors and the improvement of the superconductivity may be related to the enhanced electron-phonon coupling induced by the S-ion substitution. A dome-shaped superconducting phase diagram is obtained in the S-doped MoTe2 single crystals. MoTe2−xSx materials may provide a new platform for our understanding of superconductivity phenomena and topological physics in TMDs.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382825894045590150","@type":"Researcher","foaf:name":[{"@value":"F. C. Chen"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"},{"@value":"University of Science and Technology of China 2 , Hefei 230026, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590148","@type":"Researcher","foaf:name":[{"@value":"X. Luo"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590277","@type":"Researcher","foaf:name":[{"@value":"R. C. Xiao"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"},{"@value":"University of Science and Technology of China 2 , Hefei 230026, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590273","@type":"Researcher","foaf:name":[{"@value":"W. J. Lu"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590147","@type":"Researcher","foaf:name":[{"@value":"B. Zhang"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 3 Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, , Beijing 100190, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590144","@type":"Researcher","foaf:name":[{"@value":"H. X. Yang"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 3 Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, , Beijing 100190, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590149","@type":"Researcher","foaf:name":[{"@value":"J. Q. Li"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 3 Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, , Beijing 100190, China"},{"@value":"Collaborative Innovation Center of Quantum Matter 4 , Beijing 100190, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590146","@type":"Researcher","foaf:name":[{"@value":"Q. L. Pei"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590274","@type":"Researcher","foaf:name":[{"@value":"D. F. Shao"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590278","@type":"Researcher","foaf:name":[{"@value":"R. R. Zhang"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 5 High Magnetic Field Laboratory, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590275","@type":"Researcher","foaf:name":[{"@value":"L. S. Ling"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 5 High Magnetic Field Laboratory, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590272","@type":"Researcher","foaf:name":[{"@value":"C. Y. Xi"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 5 High Magnetic Field Laboratory, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590276","@type":"Researcher","foaf:name":[{"@value":"W. H. Song"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825894045590145","@type":"Researcher","foaf:name":[{"@value":"Y. P. Sun"}],"jpcoar:affiliationName":[{"@value":"Chinese Academy of Sciences 5 High Magnetic Field Laboratory, , Hefei 230031, China"},{"@value":"Chinese Academy of Sciences 1 Key Laboratory of Materials Physics, Institute of Solid State Physics, , Hefei 230031, China"},{"@value":"Nanjing University 6 Collaborative Innovation Center of Advanced Microstructures, , Nanjing 210093, China"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00036951"},{"@type":"EISSN","@value":"10773118"}],"prism:publicationName":[{"@value":"Applied Physics Letters"}],"dc:publisher":[{"@value":"AIP Publishing"}],"prism:publicationDate":"2016-04-18","prism:volume":"108","prism:number":"16"},"reviewed":"false","url":[{"@id":"https://pubs.aip.org/aip/apl/article-pdf/doi/10.1063/1.4947433/13865865/162601_1_online.pdf"}],"createdAt":"2016-04-20","modifiedAt":"2023-06-17","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050289920561240192","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Visualizing superconductivity in a doped Weyl semimetal with broken inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004234989647104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>MoTe</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298755611680768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Coexistence of spontaneous polarization and superconductivity in hole-doped oxyhydrides \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi>A</mml:mi><mml:mi>Ti</mml:mi><mml:msub><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mi mathvariant=\"normal\">H</mml:mi></mml:mrow></mml:math>\n (\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant=\"normal\">K</mml:mi><mml:mo>,</mml:mo><mml:mi>Rb</mml:mi><mml:mo>,</mml:mo><mml:mi>Cs</mml:mi></mml:mrow></mml:math>\n): First-principles study"}]},{"@id":"https://cir.nii.ac.jp/crid/1390571547634516608","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Mechanism of Oxygen Reduction Reaction on Monolayer WTe<sub>2</sub> with and without S Dopant at Low Coverage"}]},{"@id":"https://cir.nii.ac.jp/crid/1520854805696294272","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Pressure Induced Topological Quantum Phase Transition in Weyl Semimetal T[d]-MoTe₂"}]},{"@id":"https://cir.nii.ac.jp/crid/1523669555946330368","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Superconductivity of the Stuffed CdI₂-type Pt[1+x]Bi₂"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1063/1.4947433"},{"@type":"CROSSREF","@value":"10.1103/physrevb.95.100501_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.094707_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"},{"@type":"CROSSREF","@value":"10.1103/physrevb.104.115102_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"},{"@type":"CROSSREF","@value":"10.1103/physrevmaterials.5.054802_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"},{"@type":"CROSSREF","@value":"10.7566/jpsj.90.063706_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"},{"@type":"CROSSREF","@value":"10.1380/ejssnt.2021.119_references_DOI_T9RxcoxupVaFLLNKqzyy5wRrf9o"}]}