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氢掺杂立方氮化硼是在常压下实现120K以上高温超导的一条有前景的途径。

Hydrogen-Doped c-BN as a Promising Path to High-Temperature Superconductivity Above 120 K at Ambient Pressure.

作者信息

Ding Han-Bin, Niu Rui, Li Shen-Ao, Liu Ying-Ming, Chen Xiao-Jia, Lin Hai-Qing, Zhong Guo-Hua

机构信息

Shenzhen Institute of Advanced Technology, Chinese Academy of Sciences, Shenzhen, 518055, China.

Nano Science and Technology Institute, University of Science and Technology of China, Suzhou, 215123, China.

出版信息

Adv Sci (Weinh). 2024 Nov;11(44):e2408275. doi: 10.1002/advs.202408275. Epub 2024 Oct 7.

DOI:10.1002/advs.202408275
PMID:39373385
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11600296/
Abstract

Finding high-temperature superconductivity in light-weight element containing compounds at atmosphere pressure is currently a research hotspot but has not been reached yet. Here it is proposed that hard or superhard materials can be promising candidates to possess the desirable high-temperature superconductivity. By studying the electronic structures and superconducting properties of H and Li doped c-BN within the framework of the first-principles, it is demonstrated that the doped c-BN are indeed good superconductors at ambient pressure after undergoing the phase transition from the insulating to metallic behavior, though holding different nature of metallization. Li doped c-BN is predicted to exhibit the superconducting transition temperature of ≈58 K, while H doped c-BN has stronger electron-phonon interaction and possesses a higher transition temperature of 122 K. These results and findings thus point out a new direction for exploring the ambient-pressure higher-temperature superconductivity in hard or superhard materials.

摘要

在常压下含轻元素化合物中寻找高温超导性是当前的一个研究热点,但尚未实现。本文提出,硬材料或超硬材料有望成为具有理想高温超导性的候选材料。通过在第一性原理框架下研究H和Li掺杂立方氮化硼的电子结构和超导性能,结果表明,掺杂立方氮化硼在从绝缘态转变为金属态后,在常压下确实是良好的超导体,尽管具有不同的金属化性质。预测Li掺杂立方氮化硼的超导转变温度约为58K,而H掺杂立方氮化硼具有更强的电子-声子相互作用,其转变温度更高,为122K。这些结果和发现为探索硬材料或超硬材料中的常压高温超导性指明了一个新方向。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/63fcdc875652/ADVS-11-2408275-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/a5d5f414d55c/ADVS-11-2408275-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/3f6741d7e431/ADVS-11-2408275-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/fda063d65014/ADVS-11-2408275-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/95753782a6cd/ADVS-11-2408275-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/d6276fb6c0f7/ADVS-11-2408275-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/63fcdc875652/ADVS-11-2408275-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/a5d5f414d55c/ADVS-11-2408275-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/3f6741d7e431/ADVS-11-2408275-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/fda063d65014/ADVS-11-2408275-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/95753782a6cd/ADVS-11-2408275-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/d6276fb6c0f7/ADVS-11-2408275-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/446d/11600296/63fcdc875652/ADVS-11-2408275-g006.jpg

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