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Nematic and chiral superconductivity emerging within the loop-current phase in kagome metals

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arxiv 2508.04433 v2 pith:M2JUZDGT submitted 2025-08-06 cond-mat.supr-con cond-mat.str-el

Nematic and chiral superconductivity emerging within the loop-current phase in kagome metals

classification cond-mat.supr-con cond-mat.str-el
keywords chiralsuperconductivitykagomeloop-currentmetalsexoticnematicstate
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The kagome metals $A$V$_3$Sb$_5$ ($A =$ Cs, Rb, K) host multiple symmetry-breaking phases, including charge-density-wave and loop-current orders, and exhibit highly exotic superconductivity with pronounced nematicity and chirality. Remarkably, even dilute impurities transform this exotic superconducting state into an isotropic $s$-wave state. These observations pose a challenge to existing theoretical scenarios. We show that loop-current order induces nematic chiral $d$-wave superconductivity in kagome metals. The loop-current-induced orbital magnetization (OM) stabilizes one chiral superconducting channels. This OM-chirality coupling mechanism is generic and applies to pairing driven by either attractive or repulsive interactions. Furthermore, coexisting loop-current and bond orders give rise to pronounced nematic chiral superconductivity even for an almost $C_6$-symmetric Fermi surface. For attractive pairing, dilute impurities suppress the chiral state and restore a conventional $s$-wave phase, as observed experimentally. The theory further predicts a robust $2\times2$ pair-density modulation. This study provides key insights into time-reversal-symmetry-breaking exotic superconductivity in kagome metals.

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Cited by 2 Pith papers

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  1. NMR evidence for a loop-current state with broken $C_6$ symmetry in the charge-ordered CsV$_3$Sb$_5$

    cond-mat.supr-con 2026-06 unverdicted novelty 6.0

    NMR measurements provide evidence for a static loop-current state breaking C6 symmetry in the CDW phase of CsV3Sb5, with an internal magnetic field of 3.6 Oe at V sites and orbital moments of 0.002-0.01 μB.

  2. Scalar-spin-chirality-driven fractional Chern insulator on a kagome lattice

    cond-mat.mes-hall 2026-07 conditional novelty 5.0

    A ν=1/3 fractional Chern insulator appears in a chirality-driven kagome magnet, and stronger interactions broaden the scalar-spin-chirality range over which it remains stable.