Fully-gapped superconductivity with rotational symmetry breaking in pressurized kagome metal CsV<sub>3</sub>Sb<sub>5</sub>.
basic_science · Level V
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- Record sourced from PubMed, PMID 40240766.
- Also identified by DOI 10.1038/s41467-025-58941-w and PMC identifier 12003820.
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Abstract
The discovery of the kagome metal CsV<sub>3</sub>Sb<sub>5</sub> has generated significant interest in its complex physical properties, particularly its superconducting behavior under different pressures, though its nature remains debated. Here, we performed low-temperature, high-pressure <sup>121/123</sup>Sb nuclear quadrupole resonance (NQR) measurements to explore the superconducting pairing symmetry in CsV<sub>3</sub>Sb<sub>5</sub>. At ambient pressure, we found that the spin-lattice relaxation rate 1/T<sub>1</sub> exhibits a kink at T ~ 0.4 T<sub>c</sub> within the superconducting state and follows a T<sup>3</sup> variation as temperature further decreases. This suggests the presence of two superconducting gaps with line nodes in the smaller one. As pressure increases beyond P<sub>c</sub> ~ 1.85 GPa, where the charge-density wave phase is completely suppressed, 1/T<sub>1</sub> shows no Hebel-Slichter peak just below T<sub>c</sub>, and decreases rapidly, even faster than T<sup>5</sup>, indicating that the gap is fully opened for pressures above P<sub>c</sub>. In this high pressure region, the angular dependence of the in-plane upper critical magnetic field H<sub>c2</sub> breaks the C<sub>6</sub> rotational symmetry. We propose the s + id pairing at P > P<sub>c</sub> which explains both the 1/T<sub>1</sub> and H<sub>c2</sub> behaviors. Our findings indicate that CsV<sub>3</sub>Sb<sub>5</sub> is an unconventional superconductor and its superconducting state is even more exotic at high pressures.