论文标题
UTE2中相关的正常状态费米学和拓扑超导性
Correlated normal state fermiology and topological superconductivity in UTe2
论文作者
论文摘要
UTE2是自旋三个超导体的有前途的候选者,其中顺磁正常状态由于自旋波动而变为超导。随后发现各种异常超导性能的发现,促进了UTE2作为一个令人兴奋的操场来研究非常规的超导性,但是对正常状态的费米学及其对超导性的影响仍然需要进一步研究。在这里,我们从理论上表明,电子相关性引起了正常状态费米学的急剧变化,而在低温下由昆多共振驱动的新出现相关的费米表面(FS)。这种紧急的相关FS可以以统一的方式来解释各种非常规的超导性能。特别是,相关FS的几何形状可以自然地托管拓扑超导,在存在奇数配对的情况下,由于强烈的铁磁自旋波动,它们成为领先的不稳定。此外,两对奇数通道出现为意外退化的溶液,它们可以自然地解释具有破裂的时间反向对称性的多组分超导性。有趣的是,所得的时间反转超导态是一个Weyl超导体,其中Weyl点沿相关FS迁移,因为几乎退化配对溶液的相对大小都会有所不同。我们认为,我们发现的相关正常状态费米学提供了一个统一的平台来描述UTE2中非常规超导性。
UTe2 is a promising candidate for spin-triplet superconductors, in which a paramagnetic normal state becomes superconducting due to spin fluctuations. The subsequent discovery of various unusual superconducting properties has promoted the use of UTe2 as an exciting playground to study unconventional superconductivity, but fathoming the normal state fermiology and its influence on the superconductivity still requires further investigation. Here, we theoretically show that electron correlation induces a dramatic change in the normal state fermiology with an emergent correlated Fermi surface (FS) driven by Kondo resonance at low temperatures. This emergent correlated FS can account for various unconventional superconducting properties in a unified way. In particular, the geometry of the correlated FS can naturally host topological superconductivity in the presence of odd-parity pairings, which become the leading instability due to strong ferromagnetic spin fluctuations. Moreover, two pairs of odd-parity channels appear as accidentally degenerate solutions, which can naturally explain the multicomponent superconductivity with broken time-reversal symmetry. Interestingly, the resulting time-reversal breaking superconducting state is a Weyl superconductor in which Weyl points migrate along the correlated FS as the relative magnitude of nearly degenerate pairing solutions varies. We believe that the correlated normal state fermiology we discovered provides a unified platform to describe the unconventional superconductivity in UTe2.