{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:3BKSWD7HERJHUQZMX76UAHPMKJ","short_pith_number":"pith:3BKSWD7H","schema_version":"1.0","canonical_sha256":"d8552b0fe724527a432cbffd401dec52724a7431776d313d07ff2f96eb3fccd8","source":{"kind":"arxiv","id":"2107.04545","version":2},"attestation_state":"computed","paper":{"title":"Revealing the competition between charge-density wave and superconductivity in CsV$_3$Sb$_5$ through uniaxial strain","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Amartyajyoti Saha, Brian M. Andersen, Chaowei Hu, Morten H. Christensen, Ni Ni, Rafael M. Fernandes, Tiema Qian, Turan Birol","submitted_at":"2021-07-09T17:00:01Z","abstract_excerpt":"In this paper we report the impact of uniaxial strain $\\varepsilon$ applied along the crystalline $a$ axis on the newly discovered kagome superconductor CsV$_3$Sb$_5$. At ambient conditions, CsV$_3$Sb$_5$ shows a charge-density wave (CDW) transition at $T_{\\rm CDW}=94.5$ K and superconducts below $T_C = 3.34$ K. In our study, when the uniaxial strain $\\varepsilon$ is varied from $-0.90\\%$ to $0.90\\%$, $T_C$ monotonically increases by $\\sim 33\\%$ from 3.0 K to 4.0 K, giving rise to the empirical relation $T_C (\\varepsilon)=3.4+0.56\\varepsilon+0.12\\varepsilon^2$. On the other hand, for $\\varepsi"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2107.04545","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2021-07-09T17:00:01Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"999ffe46ffb90aca55a98fb5a4cdb3195e8bd82c6c0a7226216d3303047ad443","abstract_canon_sha256":"d2e9c2662e0eef165433b1c7ba2ab0733ce0c1841c425ecbe8fcd70415c3b146"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:25:33.180180Z","signature_b64":"No29baGtTjf5Xj3XHRgqzjbo7o1mTuJHvFm3jXHFOYKopJq38U6tgLHzihb1WJ9npqVgZizEw6aBvFbmnBZqCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8552b0fe724527a432cbffd401dec52724a7431776d313d07ff2f96eb3fccd8","last_reissued_at":"2026-07-05T03:25:33.179754Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:25:33.179754Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revealing the competition between charge-density wave and superconductivity in CsV$_3$Sb$_5$ through uniaxial strain","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Amartyajyoti Saha, Brian M. Andersen, Chaowei Hu, Morten H. Christensen, Ni Ni, Rafael M. Fernandes, Tiema Qian, Turan Birol","submitted_at":"2021-07-09T17:00:01Z","abstract_excerpt":"In this paper we report the impact of uniaxial strain $\\varepsilon$ applied along the crystalline $a$ axis on the newly discovered kagome superconductor CsV$_3$Sb$_5$. At ambient conditions, CsV$_3$Sb$_5$ shows a charge-density wave (CDW) transition at $T_{\\rm CDW}=94.5$ K and superconducts below $T_C = 3.34$ K. In our study, when the uniaxial strain $\\varepsilon$ is varied from $-0.90\\%$ to $0.90\\%$, $T_C$ monotonically increases by $\\sim 33\\%$ from 3.0 K to 4.0 K, giving rise to the empirical relation $T_C (\\varepsilon)=3.4+0.56\\varepsilon+0.12\\varepsilon^2$. On the other hand, for $\\varepsi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.04545","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2107.04545/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2107.04545","created_at":"2026-07-05T03:25:33.179811+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.04545v2","created_at":"2026-07-05T03:25:33.179811+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.04545","created_at":"2026-07-05T03:25:33.179811+00:00"},{"alias_kind":"pith_short_12","alias_value":"3BKSWD7HERJH","created_at":"2026-07-05T03:25:33.179811+00:00"},{"alias_kind":"pith_short_16","alias_value":"3BKSWD7HERJHUQZM","created_at":"2026-07-05T03:25:33.179811+00:00"},{"alias_kind":"pith_short_8","alias_value":"3BKSWD7H","created_at":"2026-07-05T03:25:33.179811+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ","json":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ.json","graph_json":"https://pith.science/api/pith-number/3BKSWD7HERJHUQZMX76UAHPMKJ/graph.json","events_json":"https://pith.science/api/pith-number/3BKSWD7HERJHUQZMX76UAHPMKJ/events.json","paper":"https://pith.science/paper/3BKSWD7H"},"agent_actions":{"view_html":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ","download_json":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ.json","view_paper":"https://pith.science/paper/3BKSWD7H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.04545&json=true","fetch_graph":"https://pith.science/api/pith-number/3BKSWD7HERJHUQZMX76UAHPMKJ/graph.json","fetch_events":"https://pith.science/api/pith-number/3BKSWD7HERJHUQZMX76UAHPMKJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ/action/storage_attestation","attest_author":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ/action/author_attestation","sign_citation":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ/action/citation_signature","submit_replication":"https://pith.science/pith/3BKSWD7HERJHUQZMX76UAHPMKJ/action/replication_record"}},"created_at":"2026-07-05T03:25:33.179811+00:00","updated_at":"2026-07-05T03:25:33.179811+00:00"}