{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:M2XC7C32CGXXAFYYQ645UJBTGR","short_pith_number":"pith:M2XC7C32","schema_version":"1.0","canonical_sha256":"66ae2f8b7a11af70171887b9da2433347e910a21cf8d7cf9c316eac95d1c1ec3","source":{"kind":"arxiv","id":"cond-mat/0211062","version":2},"attestation_state":"computed","paper":{"title":"Aging at Criticality in Model C Dynamics","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrea Gambassi, Pasquale Calabrese","submitted_at":"2002-11-04T14:04:53Z","abstract_excerpt":"We study the off-equilibrium two-point critical response and correlation functions for the relaxational dynamics with a coupling to a conserved density (Model C) of the O(N) vector model. They are determined in an \\epsilon=4-d expansion for vanishing momentum. We briefly discuss their scaling behaviors and the associated scaling forms are determined up to first order in epsilon. The corresponding fluctuation-dissipation ratio has a non trivial large time limit in the aging regime and, up to one-loop order, it is the same as that of the Model A for the physically relevant case N=1. The comparis"},"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":"cond-mat/0211062","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-11-04T14:04:53Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"25ea0dffb5b2f31db8276f9cf85577f1819f482febdfe786b2dcbf3439469f01","abstract_canon_sha256":"81d6a3110153dd9967c7c1c87cd12d396242305f8807767625a489503cdd91d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:33:18.731400Z","signature_b64":"I5RHvS/Qe1Upzyvh2xiRIpvDn+8XSEnMhk2lAkB7S/cNoWYxydqiH+UTLvZynv8VpKTvY49nxMB3IvKRirHACw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66ae2f8b7a11af70171887b9da2433347e910a21cf8d7cf9c316eac95d1c1ec3","last_reissued_at":"2026-07-04T16:33:18.731001Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:33:18.731001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Aging at Criticality in Model C Dynamics","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrea Gambassi, Pasquale Calabrese","submitted_at":"2002-11-04T14:04:53Z","abstract_excerpt":"We study the off-equilibrium two-point critical response and correlation functions for the relaxational dynamics with a coupling to a conserved density (Model C) of the O(N) vector model. They are determined in an \\epsilon=4-d expansion for vanishing momentum. We briefly discuss their scaling behaviors and the associated scaling forms are determined up to first order in epsilon. The corresponding fluctuation-dissipation ratio has a non trivial large time limit in the aging regime and, up to one-loop order, it is the same as that of the Model A for the physically relevant case N=1. The comparis"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0211062","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/cond-mat/0211062/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":"cond-mat/0211062","created_at":"2026-07-04T16:33:18.731070+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0211062v2","created_at":"2026-07-04T16:33:18.731070+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0211062","created_at":"2026-07-04T16:33:18.731070+00:00"},{"alias_kind":"pith_short_12","alias_value":"M2XC7C32CGXX","created_at":"2026-07-04T16:33:18.731070+00:00"},{"alias_kind":"pith_short_16","alias_value":"M2XC7C32CGXXAFYY","created_at":"2026-07-04T16:33:18.731070+00:00"},{"alias_kind":"pith_short_8","alias_value":"M2XC7C32","created_at":"2026-07-04T16:33:18.731070+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/M2XC7C32CGXXAFYYQ645UJBTGR","json":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR.json","graph_json":"https://pith.science/api/pith-number/M2XC7C32CGXXAFYYQ645UJBTGR/graph.json","events_json":"https://pith.science/api/pith-number/M2XC7C32CGXXAFYYQ645UJBTGR/events.json","paper":"https://pith.science/paper/M2XC7C32"},"agent_actions":{"view_html":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR","download_json":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR.json","view_paper":"https://pith.science/paper/M2XC7C32","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0211062&json=true","fetch_graph":"https://pith.science/api/pith-number/M2XC7C32CGXXAFYYQ645UJBTGR/graph.json","fetch_events":"https://pith.science/api/pith-number/M2XC7C32CGXXAFYYQ645UJBTGR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR/action/storage_attestation","attest_author":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR/action/author_attestation","sign_citation":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR/action/citation_signature","submit_replication":"https://pith.science/pith/M2XC7C32CGXXAFYYQ645UJBTGR/action/replication_record"}},"created_at":"2026-07-04T16:33:18.731070+00:00","updated_at":"2026-07-04T16:33:18.731070+00:00"}