<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Roppongi M</submitter><funding>MEXT | Japan Society for the Promotion of Science</funding><funding>MEXT | Japan Science and Technology Agency (JST)</funding><funding>MEXT | Japan Society for the Promotion of Science (JSPS)</funding><funding>National Science Foundation (NSF)</funding><funding>National Science Foundation</funding><funding>MEXT | Japan Science and Technology Agency</funding><pagination>667</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9905511</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>14(1)</volume><pubmed_abstract>The recently discovered kagome superconductors AV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> (A = K, Rb, Cs) exhibit unusual charge-density-wave (CDW) orders with time-reversal and rotational symmetry breaking. One of the most crucial unresolved issues is identifying the symmetry of the superconductivity that develops inside the CDW phase. Theory predicts a variety of unconventional superconducting symmetries with sign-changing and chiral order parameters. Experimentally, however, superconducting phase information in AV&lt;sub&gt;3&lt;/sub>Sb&lt;sub>5&lt;/sub> is still lacking. Here we report the impurity effects in CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> using electron irradiation as a phase-sensitive probe of superconductivity. Our magnetic penetration depth measurements reveal that with increasing impurities, an anisotropic fully-gapped state changes to an isotropic full-gap state without passing through a nodal state. Furthermore, transport measurements under pressure show that the double superconducting dome in the pressure-temperature phase diagram survives against sufficient impurities. These results support that CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> is a non-chiral, anisotropic s-wave superconductor with no sign change both at ambient and under pressure.</pubmed_abstract><journal>Nature communications</journal><pubmed_title>Bulk evidence of anisotropic s-wave pairing with no sign change in the kagome superconductor CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub>.</pubmed_title><pmcid>PMC9905511</pmcid><funding_grant_id>JP18KK0375</funding_grant_id><funding_grant_id>JP21H01793</funding_grant_id><funding_grant_id>DMR-1906325</funding_grant_id><funding_grant_id>JPMJCR19T5</funding_grant_id><funding_grant_id>JP20H05869</funding_grant_id><funding_grant_id>JP19H05824</funding_grant_id><funding_grant_id>JP22K18683</funding_grant_id><funding_grant_id>JP19H00649</funding_grant_id><funding_grant_id>JP22H00105</funding_grant_id><funding_grant_id>JP22K18681</funding_grant_id><funding_grant_id>JP22K20349</funding_grant_id><funding_grant_id>JP18H05227</funding_grant_id><funding_grant_id>JP22J21896</funding_grant_id><pubmed_authors>Mukasa K</pubmed_authors><pubmed_authors>Ogawa K</pubmed_authors><pubmed_authors>Ishihara K</pubmed_authors><pubmed_authors>Okada K</pubmed_authors><pubmed_authors>Grasset R</pubmed_authors><pubmed_authors>Liu S</pubmed_authors><pubmed_authors>Shibauchi T</pubmed_authors><pubmed_authors>Tanaka Y</pubmed_authors><pubmed_authors>Konczykowski M</pubmed_authors><pubmed_authors>Roppongi M</pubmed_authors><pubmed_authors>Mizukami Y</pubmed_authors><pubmed_authors>Wilson SD</pubmed_authors><pubmed_authors>Uwatoko Y</pubmed_authors><pubmed_authors>Ortiz BR</pubmed_authors><pubmed_authors>Hashimoto K</pubmed_authors></additional><is_claimable>false</is_claimable><name>Bulk evidence of anisotropic s-wave pairing with no sign change in the kagome superconductor CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub>.</name><description>The recently discovered kagome superconductors AV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> (A = K, Rb, Cs) exhibit unusual charge-density-wave (CDW) orders with time-reversal and rotational symmetry breaking. One of the most crucial unresolved issues is identifying the symmetry of the superconductivity that develops inside the CDW phase. Theory predicts a variety of unconventional superconducting symmetries with sign-changing and chiral order parameters. Experimentally, however, superconducting phase information in AV&lt;sub&gt;3&lt;/sub>Sb&lt;sub>5&lt;/sub> is still lacking. Here we report the impurity effects in CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> using electron irradiation as a phase-sensitive probe of superconductivity. Our magnetic penetration depth measurements reveal that with increasing impurities, an anisotropic fully-gapped state changes to an isotropic full-gap state without passing through a nodal state. Furthermore, transport measurements under pressure show that the double superconducting dome in the pressure-temperature phase diagram survives against sufficient impurities. These results support that CsV&lt;sub>3&lt;/sub>Sb&lt;sub>5&lt;/sub> is a non-chiral, anisotropic s-wave superconductor with no sign change both at ambient and under pressure.</description><dates><release>2023-01-01T00:00:00Z</release><publication>2023 Feb</publication><modification>2025-04-04T23:52:42.845Z</modification><creation>2025-04-04T23:52:42.845Z</creation></dates><accession>S-EPMC9905511</accession><cross_references><pubmed>36750576</pubmed><doi>10.1038/s41467-023-36273-x</doi></cross_references></HashMap>