{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:OBB6MDR5JA5LOVXRIYRDBQGB7Q","short_pith_number":"pith:OBB6MDR5","schema_version":"1.0","canonical_sha256":"7043e60e3d483ab756f1462230c0c1fc0cdf5fad021f6eb2df0cce283ea091e2","source":{"kind":"arxiv","id":"0801.1381","version":1},"attestation_state":"computed","paper":{"title":"Fluctuation-dissipation relations in critical coarsening: crossover from unmagnetized to magnetized initial states","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Alessia Annibale, Peter Sollich","submitted_at":"2008-01-09T11:36:22Z","abstract_excerpt":"We study the non-equilibrium dynamics of the spherical ferromagnet quenched to its critical temperature, as a function of the magnetization of the initial state. The two limits of unmagnetized and fully magnetized initial conditions can be understood as corresponding to times that are respectively much shorter and much longer than a magnetization timescale, as in a recent field theoretical analysis of the $n$-vector model. We calculate exactly the crossover functions interpolating between these two limits, for the magnetization correlator and response and the resulting fluctuation-dissipation "},"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":"0801.1381","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"2008-01-09T11:36:22Z","cross_cats_sorted":[],"title_canon_sha256":"327399f5bc6afa0c15e453e1ef8385e5b47ec4a9c306defa08885b7e461f2ffe","abstract_canon_sha256":"cf8ab1c1a12d81a67ca1f8f2f1f6c3ede272dedf07adbb4590ad789b198479d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:08:22.978282Z","signature_b64":"rJpqxkmkUy2NeN6ZD9u7+Wc/2HTEkA5oKnRt49eFE+r5tsDfqBjkw1kj5K7CNPRaBdJz281G54jz34URO99qBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7043e60e3d483ab756f1462230c0c1fc0cdf5fad021f6eb2df0cce283ea091e2","last_reissued_at":"2026-07-04T17:08:22.977856Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:08:22.977856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fluctuation-dissipation relations in critical coarsening: crossover from unmagnetized to magnetized initial states","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Alessia Annibale, Peter Sollich","submitted_at":"2008-01-09T11:36:22Z","abstract_excerpt":"We study the non-equilibrium dynamics of the spherical ferromagnet quenched to its critical temperature, as a function of the magnetization of the initial state. The two limits of unmagnetized and fully magnetized initial conditions can be understood as corresponding to times that are respectively much shorter and much longer than a magnetization timescale, as in a recent field theoretical analysis of the $n$-vector model. We calculate exactly the crossover functions interpolating between these two limits, for the magnetization correlator and response and the resulting fluctuation-dissipation "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0801.1381","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/0801.1381/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":"0801.1381","created_at":"2026-07-04T17:08:22.977915+00:00"},{"alias_kind":"arxiv_version","alias_value":"0801.1381v1","created_at":"2026-07-04T17:08:22.977915+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0801.1381","created_at":"2026-07-04T17:08:22.977915+00:00"},{"alias_kind":"pith_short_12","alias_value":"OBB6MDR5JA5L","created_at":"2026-07-04T17:08:22.977915+00:00"},{"alias_kind":"pith_short_16","alias_value":"OBB6MDR5JA5LOVXR","created_at":"2026-07-04T17:08:22.977915+00:00"},{"alias_kind":"pith_short_8","alias_value":"OBB6MDR5","created_at":"2026-07-04T17:08:22.977915+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/OBB6MDR5JA5LOVXRIYRDBQGB7Q","json":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q.json","graph_json":"https://pith.science/api/pith-number/OBB6MDR5JA5LOVXRIYRDBQGB7Q/graph.json","events_json":"https://pith.science/api/pith-number/OBB6MDR5JA5LOVXRIYRDBQGB7Q/events.json","paper":"https://pith.science/paper/OBB6MDR5"},"agent_actions":{"view_html":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q","download_json":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q.json","view_paper":"https://pith.science/paper/OBB6MDR5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0801.1381&json=true","fetch_graph":"https://pith.science/api/pith-number/OBB6MDR5JA5LOVXRIYRDBQGB7Q/graph.json","fetch_events":"https://pith.science/api/pith-number/OBB6MDR5JA5LOVXRIYRDBQGB7Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q/action/storage_attestation","attest_author":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q/action/author_attestation","sign_citation":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q/action/citation_signature","submit_replication":"https://pith.science/pith/OBB6MDR5JA5LOVXRIYRDBQGB7Q/action/replication_record"}},"created_at":"2026-07-04T17:08:22.977915+00:00","updated_at":"2026-07-04T17:08:22.977915+00:00"}