{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5M3T57BIVITHI42GXXDQFUKCIV","short_pith_number":"pith:5M3T57BI","schema_version":"1.0","canonical_sha256":"eb373efc28aa26747346bdc702d142454e54118b12eaadd3090dd7159fb0fd89","source":{"kind":"arxiv","id":"1210.0133","version":3},"attestation_state":"computed","paper":{"title":"Nonthermal antiferromagnetic order and nonequilibrium criticality in the Hubbard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Martin Eckstein, Naoto Tsuji, Philipp Werner","submitted_at":"2012-09-29T17:20:56Z","abstract_excerpt":"We study dynamical phase transitions from antiferromagnetic to paramagnetic states driven by an interaction quench in the fermionic Hubbard model using the nonequilibrium dynamical mean-field theory. We identify two dynamical transition points where the relaxation behavior qualitatively changes: one corresponds to the thermal phase transition at which the order parameter decays critically slowly in a power law $\\propto t^{-1/2}$, and the other is connected to the existence of nonthermal antiferromagnetic order in systems with effective temperature above the thermal critical temperature. The fr"},"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":"1210.0133","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-29T17:20:56Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"173eb9da83bf2e780c96d6c7ef8c5b42c919ad73a8eaf20ceb2526db4934d232","abstract_canon_sha256":"887a3782f21191e181d6669719ebbbeabc80d8d9945157155475c59da8bd11e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:28:05.651293Z","signature_b64":"rVIfYtH7uPR8j+JqZJdijG/ljDHLQlcRoBpCm5gQ3DJQ26w0jXmt/zhpxfGuLkaf+68C+hhJFCjIm4HIydyJDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb373efc28aa26747346bdc702d142454e54118b12eaadd3090dd7159fb0fd89","last_reissued_at":"2026-05-18T03:28:05.650581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:28:05.650581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonthermal antiferromagnetic order and nonequilibrium criticality in the Hubbard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Martin Eckstein, Naoto Tsuji, Philipp Werner","submitted_at":"2012-09-29T17:20:56Z","abstract_excerpt":"We study dynamical phase transitions from antiferromagnetic to paramagnetic states driven by an interaction quench in the fermionic Hubbard model using the nonequilibrium dynamical mean-field theory. We identify two dynamical transition points where the relaxation behavior qualitatively changes: one corresponds to the thermal phase transition at which the order parameter decays critically slowly in a power law $\\propto t^{-1/2}$, and the other is connected to the existence of nonthermal antiferromagnetic order in systems with effective temperature above the thermal critical temperature. The fr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0133","kind":"arxiv","version":3},"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":"1210.0133","created_at":"2026-05-18T03:28:05.650669+00:00"},{"alias_kind":"arxiv_version","alias_value":"1210.0133v3","created_at":"2026-05-18T03:28:05.650669+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0133","created_at":"2026-05-18T03:28:05.650669+00:00"},{"alias_kind":"pith_short_12","alias_value":"5M3T57BIVITH","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"5M3T57BIVITHI42G","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"5M3T57BI","created_at":"2026-05-18T12:26:56.085431+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/5M3T57BIVITHI42GXXDQFUKCIV","json":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV.json","graph_json":"https://pith.science/api/pith-number/5M3T57BIVITHI42GXXDQFUKCIV/graph.json","events_json":"https://pith.science/api/pith-number/5M3T57BIVITHI42GXXDQFUKCIV/events.json","paper":"https://pith.science/paper/5M3T57BI"},"agent_actions":{"view_html":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV","download_json":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV.json","view_paper":"https://pith.science/paper/5M3T57BI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1210.0133&json=true","fetch_graph":"https://pith.science/api/pith-number/5M3T57BIVITHI42GXXDQFUKCIV/graph.json","fetch_events":"https://pith.science/api/pith-number/5M3T57BIVITHI42GXXDQFUKCIV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV/action/storage_attestation","attest_author":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV/action/author_attestation","sign_citation":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV/action/citation_signature","submit_replication":"https://pith.science/pith/5M3T57BIVITHI42GXXDQFUKCIV/action/replication_record"}},"created_at":"2026-05-18T03:28:05.650669+00:00","updated_at":"2026-05-18T03:28:05.650669+00:00"}