{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:Y72RFMBEO5GMFFGWC3JQSWWMOB","short_pith_number":"pith:Y72RFMBE","schema_version":"1.0","canonical_sha256":"c7f512b024774cc294d616d3095acc70599f9cc385925abaa6997e9cd93c446f","source":{"kind":"arxiv","id":"2406.09433","version":1},"attestation_state":"computed","paper":{"title":"Kibble-Zurek Mechanism and Beyond: Lessons from a Holographic Superfluid Disk","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-th","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Adolfo del Campo, Andr\\'as Grabarits, Chuan-Yin Xia, Hua-Bi Zeng","submitted_at":"2024-06-07T09:45:37Z","abstract_excerpt":"The superfluid phase transition dynamics and associated spontaneous vortex formation with the crossing of the critical temperature in a disk geometry is studied in the framework of the $AdS/CFT$ correspondence by solving the Einstein-Abelian-Higgs model in an $AdS_4$ black hole. For a slow quench, the vortex density admits a universal scaling law with the cooling rate as predicted by the Kibble-Zurek mechanism (KZM), while for fast quenches, the density shows a universal scaling behavior as a function of the final temperature, that lies beyond the KZM prediction. The vortex number distribution"},"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":"2406.09433","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2024-06-07T09:45:37Z","cross_cats_sorted":["cond-mat.quant-gas","hep-th","quant-ph"],"title_canon_sha256":"71d16b57093b246a131e7c1940f06c32c57ccc034467e67288afb479cb6e8139","abstract_canon_sha256":"ef39272ba1fc846c53973ba9f3a244dad116fb4060b019892c74d1c94e2adb4b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-10T01:09:11.749548Z","signature_b64":"4cuS3PPfRdd8sLQ9k/wBfb3Tcq1Ik1rWO42eMGaELw2iNrtb/DGpoJI/k30BMan5UIqGJf35rfL1bA05YUVeDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7f512b024774cc294d616d3095acc70599f9cc385925abaa6997e9cd93c446f","last_reissued_at":"2026-06-10T01:09:11.748469Z","signature_status":"signed_v1","first_computed_at":"2026-06-10T01:09:11.748469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kibble-Zurek Mechanism and Beyond: Lessons from a Holographic Superfluid Disk","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-th","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Adolfo del Campo, Andr\\'as Grabarits, Chuan-Yin Xia, Hua-Bi Zeng","submitted_at":"2024-06-07T09:45:37Z","abstract_excerpt":"The superfluid phase transition dynamics and associated spontaneous vortex formation with the crossing of the critical temperature in a disk geometry is studied in the framework of the $AdS/CFT$ correspondence by solving the Einstein-Abelian-Higgs model in an $AdS_4$ black hole. For a slow quench, the vortex density admits a universal scaling law with the cooling rate as predicted by the Kibble-Zurek mechanism (KZM), while for fast quenches, the density shows a universal scaling behavior as a function of the final temperature, that lies beyond the KZM prediction. The vortex number distribution"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.09433","kind":"arxiv","version":1},"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/2406.09433/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":"2406.09433","created_at":"2026-06-10T01:09:11.748626+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.09433v1","created_at":"2026-06-10T01:09:11.748626+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.09433","created_at":"2026-06-10T01:09:11.748626+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y72RFMBEO5GM","created_at":"2026-06-10T01:09:11.748626+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y72RFMBEO5GMFFGW","created_at":"2026-06-10T01:09:11.748626+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y72RFMBE","created_at":"2026-06-10T01:09:11.748626+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.00163","citing_title":"Phase separation seeded by Z2 and U(1) topological defects from holography","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB","json":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB.json","graph_json":"https://pith.science/api/pith-number/Y72RFMBEO5GMFFGWC3JQSWWMOB/graph.json","events_json":"https://pith.science/api/pith-number/Y72RFMBEO5GMFFGWC3JQSWWMOB/events.json","paper":"https://pith.science/paper/Y72RFMBE"},"agent_actions":{"view_html":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB","download_json":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB.json","view_paper":"https://pith.science/paper/Y72RFMBE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.09433&json=true","fetch_graph":"https://pith.science/api/pith-number/Y72RFMBEO5GMFFGWC3JQSWWMOB/graph.json","fetch_events":"https://pith.science/api/pith-number/Y72RFMBEO5GMFFGWC3JQSWWMOB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB/action/storage_attestation","attest_author":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB/action/author_attestation","sign_citation":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB/action/citation_signature","submit_replication":"https://pith.science/pith/Y72RFMBEO5GMFFGWC3JQSWWMOB/action/replication_record"}},"created_at":"2026-06-10T01:09:11.748626+00:00","updated_at":"2026-06-10T01:09:11.748626+00:00"}