{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:KKFYJAMH35PEBEGZ26IX6WEQOC","short_pith_number":"pith:KKFYJAMH","schema_version":"1.0","canonical_sha256":"528b848187df5e4090d9d7917f589070b0da860690d44736ecdd8e903bd4d0d5","source":{"kind":"arxiv","id":"1806.10421","version":2},"attestation_state":"computed","paper":{"title":"Temporal disorder in discontinuous non-equilibrium phase transitions: general results","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Carlos E. Fiore, Jos\\'e A. Hoyos, M. M. de Oliveira","submitted_at":"2018-06-27T11:46:02Z","abstract_excerpt":"We develop a general theory for discontinuous non-equilibrium phase transitions into an absorbing state in the presence of temporal disorder. We focus in two paradigmatic models for discontinuous transitions: the quadratic contact process (in which activation is only spread when two nearest- neighbor sites are both active) and the contact process with long-range interactions. Using simple stability arguments (supported by Monte Carlo simulations), we show that temporal disorder does not destroy the discontinuous transition in the former model. For the latter one, the first-order transition is "},"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":"1806.10421","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-27T11:46:02Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"a1d2a1e665ec4c063ae254de0ded8b8b7b8d875f7c5ca09ea59c7cc0a277ceb2","abstract_canon_sha256":"96f97541f5af59984ef6ee906748951b0aac7e41b3e15ae617416d0e42c4b17e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:04.768106Z","signature_b64":"th8faSVs6oOI3ulJlXxxNHLZe2AlAuE9zLUgpveHYCTruXeh3b/AJNL7lck4gY5MnH7ZKxItoIktBkKiP09GDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"528b848187df5e4090d9d7917f589070b0da860690d44736ecdd8e903bd4d0d5","last_reissued_at":"2026-05-18T00:05:04.767411Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:04.767411Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temporal disorder in discontinuous non-equilibrium phase transitions: general results","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Carlos E. Fiore, Jos\\'e A. Hoyos, M. M. de Oliveira","submitted_at":"2018-06-27T11:46:02Z","abstract_excerpt":"We develop a general theory for discontinuous non-equilibrium phase transitions into an absorbing state in the presence of temporal disorder. We focus in two paradigmatic models for discontinuous transitions: the quadratic contact process (in which activation is only spread when two nearest- neighbor sites are both active) and the contact process with long-range interactions. Using simple stability arguments (supported by Monte Carlo simulations), we show that temporal disorder does not destroy the discontinuous transition in the former model. For the latter one, the first-order transition is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.10421","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":"1806.10421","created_at":"2026-05-18T00:05:04.767530+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.10421v2","created_at":"2026-05-18T00:05:04.767530+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.10421","created_at":"2026-05-18T00:05:04.767530+00:00"},{"alias_kind":"pith_short_12","alias_value":"KKFYJAMH35PE","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_16","alias_value":"KKFYJAMH35PEBEGZ","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_8","alias_value":"KKFYJAMH","created_at":"2026-05-18T12:32:33.847187+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/KKFYJAMH35PEBEGZ26IX6WEQOC","json":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC.json","graph_json":"https://pith.science/api/pith-number/KKFYJAMH35PEBEGZ26IX6WEQOC/graph.json","events_json":"https://pith.science/api/pith-number/KKFYJAMH35PEBEGZ26IX6WEQOC/events.json","paper":"https://pith.science/paper/KKFYJAMH"},"agent_actions":{"view_html":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC","download_json":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC.json","view_paper":"https://pith.science/paper/KKFYJAMH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.10421&json=true","fetch_graph":"https://pith.science/api/pith-number/KKFYJAMH35PEBEGZ26IX6WEQOC/graph.json","fetch_events":"https://pith.science/api/pith-number/KKFYJAMH35PEBEGZ26IX6WEQOC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC/action/storage_attestation","attest_author":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC/action/author_attestation","sign_citation":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC/action/citation_signature","submit_replication":"https://pith.science/pith/KKFYJAMH35PEBEGZ26IX6WEQOC/action/replication_record"}},"created_at":"2026-05-18T00:05:04.767530+00:00","updated_at":"2026-05-18T00:05:04.767530+00:00"}