{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:O4ULRZQY7XEWVIYZ3N2754OX3E","short_pith_number":"pith:O4ULRZQY","schema_version":"1.0","canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","source":{"kind":"arxiv","id":"1411.7984","version":2},"attestation_state":"computed","paper":{"title":"Non-equilibrium universality in the dynamics of dissipative cold atomic gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Beatriz Olmos, Emanuele Levi, Igor Lesanovsky, Juan P. Garrahan, Matteo Marcuzzi, Weibin Li","submitted_at":"2014-11-28T19:40:50Z","abstract_excerpt":"The theory of continuous phase transitions predicts the universal collective properties of a physical system near a critical point, which for instance manifest in characteristic power-law behaviours of physical observables. The well-established concept at or near equilibrium, universality, can also characterize the physics of systems out of equilibrium. The most fundamental instance of a genuine non-equilibrium phase transition is the directed percolation universality class, where a system switches from an absorbing inactive to a fluctuating active phase. Despite being known for several decade"},"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":"1411.7984","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-11-28T19:40:50Z","cross_cats_sorted":["physics.atom-ph","quant-ph"],"title_canon_sha256":"5f10c2021a36dfe8169352f870d68490bdee911cd4f78855f9040ffad1186913","abstract_canon_sha256":"02f66331b13a1f4aa85e00102c615f65e2a3eea030fad957566de7ba7ef0134a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:00.460581Z","signature_b64":"oiHVsw1HlzmOR/3mvPSA8f5brckXLnt5kaPklAVsWDi/yQOfrFNUWfz+KwzMWJmT5qNKuFpYkP0LxnMd6srsDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","last_reissued_at":"2026-05-18T01:12:00.460156Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:00.460156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-equilibrium universality in the dynamics of dissipative cold atomic gases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Beatriz Olmos, Emanuele Levi, Igor Lesanovsky, Juan P. Garrahan, Matteo Marcuzzi, Weibin Li","submitted_at":"2014-11-28T19:40:50Z","abstract_excerpt":"The theory of continuous phase transitions predicts the universal collective properties of a physical system near a critical point, which for instance manifest in characteristic power-law behaviours of physical observables. The well-established concept at or near equilibrium, universality, can also characterize the physics of systems out of equilibrium. The most fundamental instance of a genuine non-equilibrium phase transition is the directed percolation universality class, where a system switches from an absorbing inactive to a fluctuating active phase. Despite being known for several decade"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.7984","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":"1411.7984","created_at":"2026-05-18T01:12:00.460222+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.7984v2","created_at":"2026-05-18T01:12:00.460222+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7984","created_at":"2026-05-18T01:12:00.460222+00:00"},{"alias_kind":"pith_short_12","alias_value":"O4ULRZQY7XEW","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"O4ULRZQY7XEWVIYZ","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"O4ULRZQY","created_at":"2026-05-18T12:28:41.024544+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/O4ULRZQY7XEWVIYZ3N2754OX3E","json":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E.json","graph_json":"https://pith.science/api/pith-number/O4ULRZQY7XEWVIYZ3N2754OX3E/graph.json","events_json":"https://pith.science/api/pith-number/O4ULRZQY7XEWVIYZ3N2754OX3E/events.json","paper":"https://pith.science/paper/O4ULRZQY"},"agent_actions":{"view_html":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E","download_json":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E.json","view_paper":"https://pith.science/paper/O4ULRZQY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.7984&json=true","fetch_graph":"https://pith.science/api/pith-number/O4ULRZQY7XEWVIYZ3N2754OX3E/graph.json","fetch_events":"https://pith.science/api/pith-number/O4ULRZQY7XEWVIYZ3N2754OX3E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/action/storage_attestation","attest_author":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/action/author_attestation","sign_citation":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/action/citation_signature","submit_replication":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/action/replication_record"}},"created_at":"2026-05-18T01:12:00.460222+00:00","updated_at":"2026-05-18T01:12:00.460222+00:00"}