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Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
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Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
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Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5
Journal Article

Tunable unconventional kagome superconductivity in charge ordered RbV3Sb5 and KV3Sb5

2023
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Overview
Unconventional superconductors often feature competing orders, small superfluid density, and nodal electronic pairing. While unusual superconductivity has been proposed in the kagome metals A V 3 Sb 5 , key spectroscopic evidence has remained elusive. Here we utilize pressure-tuned and ultra-low temperature muon spin spectroscopy to uncover the unconventional nature of superconductivity in RbV 3 Sb 5 and KV 3 Sb 5 . At ambient pressure, we observed time-reversal symmetry breaking charge order below T 1 * ≃ 110 K in RbV 3 Sb 5 with an additional transition at T 2 * ≃ 50 K. Remarkably, the superconducting state displays a nodal energy gap and a reduced superfluid density, which can be attributed to the competition with the charge order. Upon applying pressure, the charge-order transitions are suppressed, the superfluid density increases, and the superconducting state progressively evolves from nodal to nodeless. Once optimal superconductivity is achieved, we find a superconducting pairing state that is not only fully gapped, but also spontaneously breaks time-reversal symmetry. Our results point to unprecedented tunable nodal kagome superconductivity competing with time-reversal symmetry-breaking charge order and offer unique insights into the nature of the pairing state. The nature of the superconductivity in the kagome metals AV 3 Sb 5 (A = K, Rb, Cs) remains under debate. Here, using muon spin spectroscopy, the authors find that the superconductivity in RbV 3 Sb 5 and KV 3 Sb 5 evolves from nodal to nodeless with increasing pressure and the superconducting state breaks time-reversal symmetry after suppression of the charge order.