{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:RXHUWS6OME6W2WNMGPIXU4KHXR","short_pith_number":"pith:RXHUWS6O","schema_version":"1.0","canonical_sha256":"8dcf4b4bce613d6d59ac33d17a7147bc5c648b27af816abd345105341df59bd6","source":{"kind":"arxiv","id":"1401.1988","version":1},"attestation_state":"computed","paper":{"title":"Dynamics of the two-dimensional directed Ising model in the paramagnetic phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Claude Godreche, Michel Pleimling","submitted_at":"2014-01-09T12:50:23Z","abstract_excerpt":"We consider the non-conserved dynamics of the Ising model on the two-dimensional square lattice, where each spin is influenced preferentially by its East and North neighbours. The single-spin flip rates are such that the stationary state is Gibbsian with respect to the usual ferromagnetic Ising Hamiltonian. We show the existence, in the paramagnetic phase, of a dynamical transition between two regimes of violation of the fluctuation-dissipation theorem in the nonequilibrium stationary state: a regime of weak violation where the stationary fluctuation-dissipation ratio is finite, when the asymm"},"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":"1401.1988","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-01-09T12:50:23Z","cross_cats_sorted":[],"title_canon_sha256":"367367ed604097dc286ca76f71f4741a1e984b1c6850cc9b110282324a979107","abstract_canon_sha256":"0c098160cb5b07a2437a318a254f902e107e5b4eb3cdf098882d328b433ea519"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:00.181448Z","signature_b64":"CSqpji7xXClVwSR/tJcT3szpoCQUny7o4+isPJ5ygFRim9/rX6NySLBcoL5BOz3D6yVHih2XSJatxX1n6mZGBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8dcf4b4bce613d6d59ac33d17a7147bc5c648b27af816abd345105341df59bd6","last_reissued_at":"2026-05-18T02:32:00.181006Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:00.181006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamics of the two-dimensional directed Ising model in the paramagnetic phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Claude Godreche, Michel Pleimling","submitted_at":"2014-01-09T12:50:23Z","abstract_excerpt":"We consider the non-conserved dynamics of the Ising model on the two-dimensional square lattice, where each spin is influenced preferentially by its East and North neighbours. The single-spin flip rates are such that the stationary state is Gibbsian with respect to the usual ferromagnetic Ising Hamiltonian. We show the existence, in the paramagnetic phase, of a dynamical transition between two regimes of violation of the fluctuation-dissipation theorem in the nonequilibrium stationary state: a regime of weak violation where the stationary fluctuation-dissipation ratio is finite, when the asymm"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.1988","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":""},"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":"1401.1988","created_at":"2026-05-18T02:32:00.181067+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.1988v1","created_at":"2026-05-18T02:32:00.181067+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.1988","created_at":"2026-05-18T02:32:00.181067+00:00"},{"alias_kind":"pith_short_12","alias_value":"RXHUWS6OME6W","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"RXHUWS6OME6W2WNM","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"RXHUWS6O","created_at":"2026-05-18T12:28:46.137349+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/RXHUWS6OME6W2WNMGPIXU4KHXR","json":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR.json","graph_json":"https://pith.science/api/pith-number/RXHUWS6OME6W2WNMGPIXU4KHXR/graph.json","events_json":"https://pith.science/api/pith-number/RXHUWS6OME6W2WNMGPIXU4KHXR/events.json","paper":"https://pith.science/paper/RXHUWS6O"},"agent_actions":{"view_html":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR","download_json":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR.json","view_paper":"https://pith.science/paper/RXHUWS6O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.1988&json=true","fetch_graph":"https://pith.science/api/pith-number/RXHUWS6OME6W2WNMGPIXU4KHXR/graph.json","fetch_events":"https://pith.science/api/pith-number/RXHUWS6OME6W2WNMGPIXU4KHXR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR/action/storage_attestation","attest_author":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR/action/author_attestation","sign_citation":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR/action/citation_signature","submit_replication":"https://pith.science/pith/RXHUWS6OME6W2WNMGPIXU4KHXR/action/replication_record"}},"created_at":"2026-05-18T02:32:00.181067+00:00","updated_at":"2026-05-18T02:32:00.181067+00:00"}