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
Hauptverfasser: Zeng, Lingyong, Ji, Yi, Yu, Dongpeng, Guo, Shu, He, Yiyi, Li, Kuan, Huang, Yanhao, Zhang, Chao, Yu, Peifeng, Luo, Shaojuan, Wang, Huichao, Luo, Huixia
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container_end_page 3712
container_issue 7
container_start_page 3705
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 &gt; 0.1) can provoke disorders, inducing the reappearance of CDW orders. 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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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