Intrinsic constraint on Tc for unconventional superconductivity

IF 5.4 1区 物理与天体物理 Q2 MATERIALS SCIENCE, MULTIDISCIPLINARY
Qiong Qin, Yi-feng Yang
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Abstract

Can room temperature superconductivity be achieved in correlated materials under ambient pressure? Our answer to this billion-dollar question is probably no, at least for realistic models within the current theoretical framework. This is shown by our systematic simulations on the pairing instability of some effective models for two-dimensional superconductivity. For a square lattice model with nearest-neighbour pairing, we find a plaquette state formed of weakly-connected 2 × 2 blocks for sufficiently large pairing interaction. The superconductivity is suppressed on both sides away from its melting quantum critical point. Thus, the magnitude of Tc is constrained by the plaquette state for the d-wave superconductivity, in resemblance of other competing orders. We then extend our simulations to a variety of effective models covering nearest-neighbour or onsite pairings, single layer or two-layer structures, intralayer or interlayer pairings, and find an intrinsic maximum of the ratio Tc/J ≈ 0.04−0.07, where J is the pairing interaction, given by the onsite attractive interaction in the attractive Hubbard model or the exchange interaction in the repulsive Hubbard model. Our results agree well with previous quantum Monte Carlo simulations for the attractive Hubbard model. Comparison with existing experiments supports this constraint in cuprate, iron-based, nickelate, and heavy fermion superconductors, despite that these compounds are so complicated well beyond our simplified models. As a result, the known families of unconventional superconductivity, possibly except the infinite-layer nickelates, seem to almost exhaust their potentials in reaching the maximal Tc allowed by their respective J, while achieving room temperature superconductor would require a much larger J beyond 400–700 meV, which seems unrealistic in existing correlated materials and hence demands novel pairing mechanisms. The agreement also implies some deep underlying principles of the constraint that urge for a more rigorous theoretical understanding.

Abstract Image

非常规超导中Tc的本征约束
相关材料在环境压力下能否实现室温超导?对于这个价值数十亿美元的问题,我们的答案可能是否定的,至少对于目前理论框架内的现实模型来说是这样。我们对一些二维超导有效模型的配对不稳定性进行了系统的模拟,证明了这一点。对于具有最近邻配对的方形晶格模型,我们发现了一个由弱连接的2 × 2块构成的斑块状态,以获得足够大的配对相互作用。在远离熔融量子临界点的两侧,超导性被抑制。因此,Tc的大小受到d波超导的斑块状态的限制,类似于其他竞争阶。然后,我们将模拟扩展到涵盖最近邻或现场配对、单层或双层结构、层内或层间配对的各种有效模型,并找到比值Tc/J≈0.04−0.07的固有最大值,其中J是配对相互作用,由吸引Hubbard模型中的现场吸引相互作用或排斥Hubbard模型中的交换相互作用给出。我们的结果与先前的量子蒙特卡罗模拟相一致。在铜、铁基、镍酸盐和重费米子超导体中,与现有实验的比较支持这一限制,尽管这些化合物非常复杂,远远超出了我们的简化模型。因此,已知的非常规超导家族,可能除了无限层镍酸盐外,似乎几乎耗尽了它们达到各自J允许的最大Tc的潜力,而实现室温超导体将需要超过400-700 meV的更大的J,这在现有的相关材料中似乎是不现实的,因此需要新的配对机制。这种一致也暗示了约束的一些深层次的基本原则,这些原则要求我们进行更严格的理论理解。
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来源期刊
npj Quantum Materials
npj Quantum Materials Materials Science-Electronic, Optical and Magnetic Materials
CiteScore
10.60
自引率
3.50%
发文量
107
审稿时长
6 weeks
期刊介绍: npj Quantum Materials is an open access journal that publishes works that significantly advance the understanding of quantum materials, including their fundamental properties, fabrication and applications.
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