Negative Chemical Pressure Effect on the Superconductivity and Charge Density Wave of Cu0.5Ir1–x Zr x Te2
This study demonstrates the design and synthesis of the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system by partial substitution of Ir with Zr acting as a negative chemical pressure. With the doping of Zr, the cell parameters significantly expand, signifying an effective negative chemical pressure. The exp...
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Veröffentlicht in: | Journal of physical chemistry. C 2022-02, Vol.126 (7), p.3705-3712 |
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container_title | Journal of physical chemistry. C |
container_volume | 126 |
creator | Zeng, Lingyong Ji, Yi Yu, Dongpeng Guo, Shu He, Yiyi Li, Kuan Huang, Yanhao Zhang, Chao Yu, Peifeng Luo, Shaojuan Wang, Huichao Luo, Huixia |
description | This study demonstrates the design and synthesis of the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system by partial substitution of Ir with Zr acting as a negative chemical pressure. With the doping of Zr, the cell parameters significantly expand, signifying an effective negative chemical pressure. The experimental results find evidence that the charge density wave (CDW)-like order is immediately quenched by subtle Zr substitution for Ir and a classical dome-shape T c(x) that peaked at 2.80 K can be observed. The optimal Cu0.5Ir0.95Zr0.05Te2 compound is a Bardeen–Cooper–Schrieffer (BCS)-type superconductor and exhibits type-II superconductivity (SC). However, high Zr concentrations (x > 0.1) can provoke disorders, inducing the reappearance of CDW orders. The present study shows that the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system may provide a new platform for further understanding multiple electronic orders in transition-metal dichalcogenides. |
doi_str_mv | 10.1021/acs.jpcc.1c10092 |
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With the doping of Zr, the cell parameters significantly expand, signifying an effective negative chemical pressure. The experimental results find evidence that the charge density wave (CDW)-like order is immediately quenched by subtle Zr substitution for Ir and a classical dome-shape T c(x) that peaked at 2.80 K can be observed. The optimal Cu0.5Ir0.95Zr0.05Te2 compound is a Bardeen–Cooper–Schrieffer (BCS)-type superconductor and exhibits type-II superconductivity (SC). However, high Zr concentrations (x > 0.1) can provoke disorders, inducing the reappearance of CDW orders. The present study shows that the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system may provide a new platform for further understanding multiple electronic orders in transition-metal dichalcogenides.</description><identifier>ISSN: 1932-7447</identifier><identifier>EISSN: 1932-7455</identifier><identifier>DOI: 10.1021/acs.jpcc.1c10092</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>C: Physical Properties of Materials and Interfaces</subject><ispartof>Journal of physical chemistry. 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The present study shows that the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system may provide a new platform for further understanding multiple electronic orders in transition-metal dichalcogenides.</description><subject>C: Physical Properties of Materials and Interfaces</subject><issn>1932-7447</issn><issn>1932-7455</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqVj89qwkAQh5ei4L_ePc4D1HQmMYjnVNFLESoIXpZlnWhSu5HdrOjNd_AN-yRdRXr3NMPH7zfMJ0SfMCKM6V1pF5UHrSPShDiOX0Sbxkk8GA3TtPG_D0ct0XGuREwTpKQtvj95q-riyJDt-KfQag8Ly855yzDJc9Y1VAbqHcOXP7DVldl4HfJFfQZlNqGl7Jbhg427oZUKl6ocMo9ROrf0e7meYG3hBEuOe6KZq73j18fsirfpZJnNBuF3WVbemkAlobwJyTsMQvIhlDwZ_wMH5lUV</recordid><startdate>20220224</startdate><enddate>20220224</enddate><creator>Zeng, Lingyong</creator><creator>Ji, Yi</creator><creator>Yu, Dongpeng</creator><creator>Guo, Shu</creator><creator>He, Yiyi</creator><creator>Li, Kuan</creator><creator>Huang, Yanhao</creator><creator>Zhang, Chao</creator><creator>Yu, Peifeng</creator><creator>Luo, Shaojuan</creator><creator>Wang, Huichao</creator><creator>Luo, Huixia</creator><general>American Chemical Society</general><scope/><orcidid>https://orcid.org/0000-0003-2703-5660</orcidid><orcidid>https://orcid.org/0000-0003-3584-090X</orcidid></search><sort><creationdate>20220224</creationdate><title>Negative Chemical Pressure Effect on the Superconductivity and Charge Density Wave of Cu0.5Ir1–x Zr x Te2</title><author>Zeng, Lingyong ; Ji, Yi ; Yu, Dongpeng ; Guo, Shu ; He, Yiyi ; Li, Kuan ; Huang, Yanhao ; Zhang, Chao ; Yu, Peifeng ; Luo, Shaojuan ; Wang, Huichao ; Luo, Huixia</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-acs_journals_10_1021_acs_jpcc_1c100923</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>C: Physical Properties of Materials and Interfaces</topic><toplevel>online_resources</toplevel><creatorcontrib>Zeng, Lingyong</creatorcontrib><creatorcontrib>Ji, Yi</creatorcontrib><creatorcontrib>Yu, Dongpeng</creatorcontrib><creatorcontrib>Guo, Shu</creatorcontrib><creatorcontrib>He, Yiyi</creatorcontrib><creatorcontrib>Li, Kuan</creatorcontrib><creatorcontrib>Huang, Yanhao</creatorcontrib><creatorcontrib>Zhang, Chao</creatorcontrib><creatorcontrib>Yu, Peifeng</creatorcontrib><creatorcontrib>Luo, Shaojuan</creatorcontrib><creatorcontrib>Wang, Huichao</creatorcontrib><creatorcontrib>Luo, Huixia</creatorcontrib><jtitle>Journal of physical chemistry. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zeng, Lingyong</au><au>Ji, Yi</au><au>Yu, Dongpeng</au><au>Guo, Shu</au><au>He, Yiyi</au><au>Li, Kuan</au><au>Huang, Yanhao</au><au>Zhang, Chao</au><au>Yu, Peifeng</au><au>Luo, Shaojuan</au><au>Wang, Huichao</au><au>Luo, Huixia</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Negative Chemical Pressure Effect on the Superconductivity and Charge Density Wave of Cu0.5Ir1–x Zr x Te2</atitle><jtitle>Journal of physical chemistry. C</jtitle><addtitle>J. Phys. Chem. C</addtitle><date>2022-02-24</date><risdate>2022</risdate><volume>126</volume><issue>7</issue><spage>3705</spage><epage>3712</epage><pages>3705-3712</pages><issn>1932-7447</issn><eissn>1932-7455</eissn><abstract>This study demonstrates the design and synthesis of the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system by partial substitution of Ir with Zr acting as a negative chemical pressure. With the doping of Zr, the cell parameters significantly expand, signifying an effective negative chemical pressure. The experimental results find evidence that the charge density wave (CDW)-like order is immediately quenched by subtle Zr substitution for Ir and a classical dome-shape T c(x) that peaked at 2.80 K can be observed. The optimal Cu0.5Ir0.95Zr0.05Te2 compound is a Bardeen–Cooper–Schrieffer (BCS)-type superconductor and exhibits type-II superconductivity (SC). However, high Zr concentrations (x > 0.1) can provoke disorders, inducing the reappearance of CDW orders. The present study shows that the Cu0.5Ir1–x Zr x Te2 (0 ≤ x ≤ 0.15) system may provide a new platform for further understanding multiple electronic orders in transition-metal dichalcogenides.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.jpcc.1c10092</doi><orcidid>https://orcid.org/0000-0003-2703-5660</orcidid><orcidid>https://orcid.org/0000-0003-3584-090X</orcidid></addata></record> |
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title | Negative Chemical Pressure Effect on the Superconductivity and Charge Density Wave of Cu0.5Ir1–x Zr x Te2 |
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