On the Superconductivity in High-Entropy Alloy (NbTa)1-X(HfZrTi)X  

On the Superconductivity in High-Entropy Alloy (NbTa)1-X(HfZrTi)X

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作  者:Snehadri B. Ota Snehadri B. Ota(Government of India, New Delhi, India)

机构地区:[1]Government of India, New Delhi, India

出  处:《Journal of Modern Physics》2023年第4期445-449,共5页现代物理(英文)

摘  要:The superconductivity in (NbTa)<sub>1-X</sub>(HfZrTi)<sub>X</sub> high-entropy alloy is analyzed using the theory of strong-coupled superconductor. It is concluded that (NbTa)<sub>1-X</sub>(HfZrTi)<sub>X </sub>is a strong coupled superconductor. The variation in the superconducting transition temperature from 7.9 K to 4.6 K as x increases from 0.2 to 0.84 arises because of the decrease in electronic band width due to localization and broadening of the band. It is suggested that the decrease in electronic band width is due to crystalline randomness which gives rise to the mobility edge.The superconductivity in (NbTa)<sub>1-X</sub>(HfZrTi)<sub>X</sub> high-entropy alloy is analyzed using the theory of strong-coupled superconductor. It is concluded that (NbTa)<sub>1-X</sub>(HfZrTi)<sub>X </sub>is a strong coupled superconductor. The variation in the superconducting transition temperature from 7.9 K to 4.6 K as x increases from 0.2 to 0.84 arises because of the decrease in electronic band width due to localization and broadening of the band. It is suggested that the decrease in electronic band width is due to crystalline randomness which gives rise to the mobility edge.

关 键 词:High-Entropy Alloys Disordered Metals Strong-Coupled Superconductivity LOCALIZATION Cocktail Effect 

分 类 号:TG1[金属学及工艺—金属学]

 

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