{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:573B7HHVSIFJMDIL3PGVY7PPIA","short_pith_number":"pith:573B7HHV","schema_version":"1.0","canonical_sha256":"eff61f9cf5920a960d0bdbcd5c7def403f005871158b3bfc0efe11fb72a83fc8","source":{"kind":"arxiv","id":"2501.13177","version":1},"attestation_state":"computed","paper":{"title":"Localization of Dirac modes in a finite temperature SU(2) Higgs model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"hep-lat","authors_text":"Gy\\\"orgy Baranka, Matteo Giordano","submitted_at":"2025-01-22T19:12:05Z","abstract_excerpt":"Low-lying Dirac modes become localized at the finite-temperature transition in QCD and other gauge theories, indicating a strong connection between localization and deconfinement. This phenomenon can be understood through the \"sea/islands\" picture: in the deconfined phase, modes become trapped on \"islands\" of Polyakov loop fluctuations within a \"sea\" of ordered Polyakov loops. To test the universality of the \"sea/islands\" mechanism, we investigate whether changes in the localization properties of low modes occur across other thermal transitions where the Polyakov loop becomes ordered, beyond t"},"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":"2501.13177","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2025-01-22T19:12:05Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"77886bc3adde11cf3fd3da38d3350217fc2b109891381d9843f0968fcc3bd3c9","abstract_canon_sha256":"b42413dc22ea1d7480dc3e7cf0a6ca88bab8a8e8792151bba9878772f9dd878b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:04:24.605656Z","signature_b64":"rj7J4V/KA4Dnwfp7psKMGLU/EFHTXkKtNCbOdW0tarsvPYCyiNOoLv7ZGriuHvhiUdD+PdClalgHApz7wFUoAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eff61f9cf5920a960d0bdbcd5c7def403f005871158b3bfc0efe11fb72a83fc8","last_reissued_at":"2026-07-05T10:04:24.605157Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:04:24.605157Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Localization of Dirac modes in a finite temperature SU(2) Higgs model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"hep-lat","authors_text":"Gy\\\"orgy Baranka, Matteo Giordano","submitted_at":"2025-01-22T19:12:05Z","abstract_excerpt":"Low-lying Dirac modes become localized at the finite-temperature transition in QCD and other gauge theories, indicating a strong connection between localization and deconfinement. This phenomenon can be understood through the \"sea/islands\" picture: in the deconfined phase, modes become trapped on \"islands\" of Polyakov loop fluctuations within a \"sea\" of ordered Polyakov loops. To test the universality of the \"sea/islands\" mechanism, we investigate whether changes in the localization properties of low modes occur across other thermal transitions where the Polyakov loop becomes ordered, beyond t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.13177","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/2501.13177/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":"2501.13177","created_at":"2026-07-05T10:04:24.605212+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.13177v1","created_at":"2026-07-05T10:04:24.605212+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.13177","created_at":"2026-07-05T10:04:24.605212+00:00"},{"alias_kind":"pith_short_12","alias_value":"573B7HHVSIFJ","created_at":"2026-07-05T10:04:24.605212+00:00"},{"alias_kind":"pith_short_16","alias_value":"573B7HHVSIFJMDIL","created_at":"2026-07-05T10:04:24.605212+00:00"},{"alias_kind":"pith_short_8","alias_value":"573B7HHV","created_at":"2026-07-05T10:04:24.605212+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/573B7HHVSIFJMDIL3PGVY7PPIA","json":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA.json","graph_json":"https://pith.science/api/pith-number/573B7HHVSIFJMDIL3PGVY7PPIA/graph.json","events_json":"https://pith.science/api/pith-number/573B7HHVSIFJMDIL3PGVY7PPIA/events.json","paper":"https://pith.science/paper/573B7HHV"},"agent_actions":{"view_html":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA","download_json":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA.json","view_paper":"https://pith.science/paper/573B7HHV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.13177&json=true","fetch_graph":"https://pith.science/api/pith-number/573B7HHVSIFJMDIL3PGVY7PPIA/graph.json","fetch_events":"https://pith.science/api/pith-number/573B7HHVSIFJMDIL3PGVY7PPIA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA/action/storage_attestation","attest_author":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA/action/author_attestation","sign_citation":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA/action/citation_signature","submit_replication":"https://pith.science/pith/573B7HHVSIFJMDIL3PGVY7PPIA/action/replication_record"}},"created_at":"2026-07-05T10:04:24.605212+00:00","updated_at":"2026-07-05T10:04:24.605212+00:00"}