{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:BEFEXVRSK2Z2T53W4UB3UUAXTU","short_pith_number":"pith:BEFEXVRS","schema_version":"1.0","canonical_sha256":"090a4bd63256b3a9f776e503ba50179d3f1ef44817ddef23cc4b245bf5451fbe","source":{"kind":"arxiv","id":"2204.11627","version":2},"attestation_state":"computed","paper":{"title":"Superdiffusive quantum work and adiabatic quantum evolution in finite temperature chaotic Fermi systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andr\\'as Grabarits, Gergely Zar\\'and, Izabella Lovas, M\\'arton Kormos","submitted_at":"2022-04-25T12:58:42Z","abstract_excerpt":"We study the full distribution of quantum work in generic, noninteracting, disordered fermionic nanosystems at finite temperature. We derive an analytical determinant formula for the characteristic function of work statistics for quantum quenches starting from a thermal initial state. For work small compared to the thermal energy of the Fermi gas, work distribution is Gaussian, and the variance of work is proportional to the average work, while in the low temperature or large work limit, a non-Gaussian distribution with superdiffusive work fluctuations is observed. Similarly, the time dependen"},"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":"2204.11627","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-04-25T12:58:42Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"dd1a93ce9cd6342344c7319b77c9843daede0cd84d228a6dcb197c66adf106c3","abstract_canon_sha256":"a29929917e43e0bdeec8ae2577872a596182ecf39cc9a98d2b3caebe1028fcfb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:33:10.384612Z","signature_b64":"hgOXhtLqmHQiZj56qDGo8SHg2CbgDYXUzL3LHgyVwmpIAtUV8i6cU2I3CmOAMcZjIFponh2YKMcMpADRDhFBBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"090a4bd63256b3a9f776e503ba50179d3f1ef44817ddef23cc4b245bf5451fbe","last_reissued_at":"2026-07-05T05:33:10.384138Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:33:10.384138Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superdiffusive quantum work and adiabatic quantum evolution in finite temperature chaotic Fermi systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andr\\'as Grabarits, Gergely Zar\\'and, Izabella Lovas, M\\'arton Kormos","submitted_at":"2022-04-25T12:58:42Z","abstract_excerpt":"We study the full distribution of quantum work in generic, noninteracting, disordered fermionic nanosystems at finite temperature. We derive an analytical determinant formula for the characteristic function of work statistics for quantum quenches starting from a thermal initial state. For work small compared to the thermal energy of the Fermi gas, work distribution is Gaussian, and the variance of work is proportional to the average work, while in the low temperature or large work limit, a non-Gaussian distribution with superdiffusive work fluctuations is observed. Similarly, the time dependen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.11627","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/2204.11627/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":"2204.11627","created_at":"2026-07-05T05:33:10.384195+00:00"},{"alias_kind":"arxiv_version","alias_value":"2204.11627v2","created_at":"2026-07-05T05:33:10.384195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.11627","created_at":"2026-07-05T05:33:10.384195+00:00"},{"alias_kind":"pith_short_12","alias_value":"BEFEXVRSK2Z2","created_at":"2026-07-05T05:33:10.384195+00:00"},{"alias_kind":"pith_short_16","alias_value":"BEFEXVRSK2Z2T53W","created_at":"2026-07-05T05:33:10.384195+00:00"},{"alias_kind":"pith_short_8","alias_value":"BEFEXVRS","created_at":"2026-07-05T05:33:10.384195+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/BEFEXVRSK2Z2T53W4UB3UUAXTU","json":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU.json","graph_json":"https://pith.science/api/pith-number/BEFEXVRSK2Z2T53W4UB3UUAXTU/graph.json","events_json":"https://pith.science/api/pith-number/BEFEXVRSK2Z2T53W4UB3UUAXTU/events.json","paper":"https://pith.science/paper/BEFEXVRS"},"agent_actions":{"view_html":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU","download_json":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU.json","view_paper":"https://pith.science/paper/BEFEXVRS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2204.11627&json=true","fetch_graph":"https://pith.science/api/pith-number/BEFEXVRSK2Z2T53W4UB3UUAXTU/graph.json","fetch_events":"https://pith.science/api/pith-number/BEFEXVRSK2Z2T53W4UB3UUAXTU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU/action/storage_attestation","attest_author":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU/action/author_attestation","sign_citation":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU/action/citation_signature","submit_replication":"https://pith.science/pith/BEFEXVRSK2Z2T53W4UB3UUAXTU/action/replication_record"}},"created_at":"2026-07-05T05:33:10.384195+00:00","updated_at":"2026-07-05T05:33:10.384195+00:00"}