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富勒烯超导材料中,在莫特转变附近上临界场达到 90 特斯拉。

Upper critical field reaches 90 tesla near the Mott transition in fulleride superconductors.

机构信息

Department of Physics, Kyoto University, Kyoto 606-8502, Japan.

Quantum-Phase Electronics Center (QPEC) and Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan.

出版信息

Nat Commun. 2017 Feb 17;8:14467. doi: 10.1038/ncomms14467.

DOI:10.1038/ncomms14467
PMID:28211544
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5321754/
Abstract

Controlled access to the border of the Mott insulating state by variation of control parameters offers exotic electronic states such as anomalous and possibly high-transition-temperature (T) superconductivity. The alkali-doped fullerides show a transition from a Mott insulator to a superconductor for the first time in three-dimensional materials, but the impact of dimensionality and electron correlation on superconducting properties has remained unclear. Here we show that, near the Mott insulating phase, the upper critical field H of the fulleride superconductors reaches values as high as ∼90 T-the highest among cubic crystals. This is accompanied by a crossover from weak- to strong-coupling superconductivity and appears upon entering the metallic state with the dynamical Jahn-Teller effect as the Mott transition is approached. These results suggest that the cooperative interplay between molecular electronic structure and strong electron correlations plays a key role in realizing robust superconductivity with high-T and high-H.

摘要

通过控制参数来控制莫特绝缘状态的边界,可以提供奇异的电子态,例如异常和可能具有高转变温度(T)的超导性。 碱掺杂富勒烯首次在三维材料中从莫特绝缘体转变为超导体,但维度和电子相关对超导性质的影响仍不清楚。 在这里,我们表明,在莫特绝缘相附近,富勒烯超导体的上临界场 H 达到高达约 90 T 的值-在立方晶体中是最高的。 这伴随着从弱耦合到强耦合超导的转变,并且随着动态 Jahn-Teller 效应接近莫特转变而进入金属态时出现。 这些结果表明,分子电子结构和强电子相关之间的协同相互作用在实现具有高 T 和高 H 的稳健超导性方面起着关键作用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/bd7efcafc0bd/ncomms14467-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/6a9c117cc602/ncomms14467-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/5b8ee9cfd884/ncomms14467-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/337dfdace652/ncomms14467-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/bd7efcafc0bd/ncomms14467-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/6a9c117cc602/ncomms14467-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/5b8ee9cfd884/ncomms14467-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/337dfdace652/ncomms14467-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5823/5321754/bd7efcafc0bd/ncomms14467-f4.jpg

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