{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:43RMRNQNSRTVA4IMSDP46V7ZHT","short_pith_number":"pith:43RMRNQN","schema_version":"1.0","canonical_sha256":"e6e2c8b60d946750710c90dfcf57f93cc6416315635c39746ec06e53afa518bb","source":{"kind":"arxiv","id":"0908.1518","version":2},"attestation_state":"computed","paper":{"title":"Study of the Nonequilibrium Critical Quenching and Annealing Dynamics for the Long-Range Ising Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["stat.CO"],"primary_cat":"cond-mat.stat-mech","authors_text":"D. E. Rodriguez, E. V. Albano, M. A. Bab","submitted_at":"2009-08-11T14:37:49Z","abstract_excerpt":"Extensive Monte Carlo simulations are employed in order to study the dynamic critical behavior of the one-dimensional Ising magnet, with algebraically decaying long-range interactions of the form $\\frac{1}{r^{d+\\sigma}}$, with $\\sigma=0.75$. The critical temperature, as well as the critical exponents, is evaluated from the power-law behavior of suitable physical observables when the system is quenched from uncorrelated states, corresponding to infinite temperature, to the critical point. These results are compared with those obtained from the dynamic evolution of the system when it is suddenly"},"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":"0908.1518","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2009-08-11T14:37:49Z","cross_cats_sorted":["stat.CO"],"title_canon_sha256":"ee82bbf07dca6bcd30634b5dcc8dfc438f610aa873e7bedfa2be55d81811c888","abstract_canon_sha256":"7d446ff04fb07b9c3beb8f7f59f16bb00807f4c4d1b3d83be34ed7315d642ae7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:24:27.803993Z","signature_b64":"1fqUPD/ko/aHLnSMDnSlKhNsPU5tFmm5ebQjuyYSRg96nj5ZCb+Gj1GUsDTeTP6xGwSs8AOovyE9xN+Wit0dDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6e2c8b60d946750710c90dfcf57f93cc6416315635c39746ec06e53afa518bb","last_reissued_at":"2026-05-18T04:24:27.803420Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:24:27.803420Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Study of the Nonequilibrium Critical Quenching and Annealing Dynamics for the Long-Range Ising Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["stat.CO"],"primary_cat":"cond-mat.stat-mech","authors_text":"D. E. Rodriguez, E. V. Albano, M. A. Bab","submitted_at":"2009-08-11T14:37:49Z","abstract_excerpt":"Extensive Monte Carlo simulations are employed in order to study the dynamic critical behavior of the one-dimensional Ising magnet, with algebraically decaying long-range interactions of the form $\\frac{1}{r^{d+\\sigma}}$, with $\\sigma=0.75$. The critical temperature, as well as the critical exponents, is evaluated from the power-law behavior of suitable physical observables when the system is quenched from uncorrelated states, corresponding to infinite temperature, to the critical point. These results are compared with those obtained from the dynamic evolution of the system when it is suddenly"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1518","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":""},"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":"0908.1518","created_at":"2026-05-18T04:24:27.803502+00:00"},{"alias_kind":"arxiv_version","alias_value":"0908.1518v2","created_at":"2026-05-18T04:24:27.803502+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1518","created_at":"2026-05-18T04:24:27.803502+00:00"},{"alias_kind":"pith_short_12","alias_value":"43RMRNQNSRTV","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_16","alias_value":"43RMRNQNSRTVA4IM","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_8","alias_value":"43RMRNQN","created_at":"2026-05-18T12:25:58.018023+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/43RMRNQNSRTVA4IMSDP46V7ZHT","json":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT.json","graph_json":"https://pith.science/api/pith-number/43RMRNQNSRTVA4IMSDP46V7ZHT/graph.json","events_json":"https://pith.science/api/pith-number/43RMRNQNSRTVA4IMSDP46V7ZHT/events.json","paper":"https://pith.science/paper/43RMRNQN"},"agent_actions":{"view_html":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT","download_json":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT.json","view_paper":"https://pith.science/paper/43RMRNQN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0908.1518&json=true","fetch_graph":"https://pith.science/api/pith-number/43RMRNQNSRTVA4IMSDP46V7ZHT/graph.json","fetch_events":"https://pith.science/api/pith-number/43RMRNQNSRTVA4IMSDP46V7ZHT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT/action/storage_attestation","attest_author":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT/action/author_attestation","sign_citation":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT/action/citation_signature","submit_replication":"https://pith.science/pith/43RMRNQNSRTVA4IMSDP46V7ZHT/action/replication_record"}},"created_at":"2026-05-18T04:24:27.803502+00:00","updated_at":"2026-05-18T04:24:27.803502+00:00"}