{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:O4ULRZQY7XEWVIYZ3N2754OX3E","short_pith_number":"pith:O4ULRZQY","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"},"canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","source":{"kind":"arxiv","id":"1411.7984","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.7984","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"arxiv_version","alias_value":"1411.7984v2","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7984","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"pith_short_12","alias_value":"O4ULRZQY7XEW","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"O4ULRZQY7XEWVIYZ","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"O4ULRZQY","created_at":"2026-05-18T12:28:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:O4ULRZQY7XEWVIYZ3N2754OX3E","target":"record","payload":{"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"},"canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","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"},"source_kind":"arxiv","source_id":"1411.7984","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:12:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"er72h4fWK4tw5CvKOVBEr6Q9bbg/GHr69ODOD86uj0t9FtVT8lRHYrCuj+1oTtmntxWThuYMqGO3lVEeGjUuCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:47:43.578572Z"},"content_sha256":"e2dc4bea842dd0e19266bf770a1885d6991f942c61d5cc543d2ba146b8b361bc","schema_version":"1.0","event_id":"sha256:e2dc4bea842dd0e19266bf770a1885d6991f942c61d5cc543d2ba146b8b361bc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:O4ULRZQY7XEWVIYZ3N2754OX3E","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:12:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7jFPPwT13i9IZYRjmtk0RjdBTqWICQOIG/Hwth8me14YVvWxm4mBB6pKxZfnU89x4570+CIjNAEzjTAjaU/YAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:47:43.579217Z"},"content_sha256":"763b8618342bfe2c90a955d33f2b33f5c539922ef92e223b1056e66d48e4824f","schema_version":"1.0","event_id":"sha256:763b8618342bfe2c90a955d33f2b33f5c539922ef92e223b1056e66d48e4824f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/bundle.json","state_url":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T00:47:43Z","links":{"resolver":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E","bundle":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/bundle.json","state":"https://pith.science/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/state.json","well_known_bundle":"https://pith.science/.well-known/pith/O4ULRZQY7XEWVIYZ3N2754OX3E/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:O4ULRZQY7XEWVIYZ3N2754OX3E","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"02f66331b13a1f4aa85e00102c615f65e2a3eea030fad957566de7ba7ef0134a","cross_cats_sorted":["physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-11-28T19:40:50Z","title_canon_sha256":"5f10c2021a36dfe8169352f870d68490bdee911cd4f78855f9040ffad1186913"},"schema_version":"1.0","source":{"id":"1411.7984","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.7984","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"arxiv_version","alias_value":"1411.7984v2","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7984","created_at":"2026-05-18T01:12:00Z"},{"alias_kind":"pith_short_12","alias_value":"O4ULRZQY7XEW","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"O4ULRZQY7XEWVIYZ","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"O4ULRZQY","created_at":"2026-05-18T12:28:41Z"}],"graph_snapshots":[{"event_id":"sha256:763b8618342bfe2c90a955d33f2b33f5c539922ef92e223b1056e66d48e4824f","target":"graph","created_at":"2026-05-18T01:12:00Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"Beatriz Olmos, Emanuele Levi, Igor Lesanovsky, Juan P. Garrahan, Matteo Marcuzzi, Weibin Li","cross_cats":["physics.atom-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-11-28T19:40:50Z","title":"Non-equilibrium universality in the dynamics of dissipative cold atomic gases"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.7984","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:e2dc4bea842dd0e19266bf770a1885d6991f942c61d5cc543d2ba146b8b361bc","target":"record","created_at":"2026-05-18T01:12:00Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"02f66331b13a1f4aa85e00102c615f65e2a3eea030fad957566de7ba7ef0134a","cross_cats_sorted":["physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-11-28T19:40:50Z","title_canon_sha256":"5f10c2021a36dfe8169352f870d68490bdee911cd4f78855f9040ffad1186913"},"schema_version":"1.0","source":{"id":"1411.7984","kind":"arxiv","version":2}},"canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7728b8e618fdc96aa319db75fef1d7d90c4093434dbb0c786435c7b665070179","first_computed_at":"2026-05-18T01:12:00.460156Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:00.460156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oiHVsw1HlzmOR/3mvPSA8f5brckXLnt5kaPklAVsWDi/yQOfrFNUWfz+KwzMWJmT5qNKuFpYkP0LxnMd6srsDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:00.460581Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.7984","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e2dc4bea842dd0e19266bf770a1885d6991f942c61d5cc543d2ba146b8b361bc","sha256:763b8618342bfe2c90a955d33f2b33f5c539922ef92e223b1056e66d48e4824f"],"state_sha256":"06f60a99070e9b947a33e5d23b6027650e35e81e3e7fd4c9c16b9e88a8c4e22a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nuMFycsCPoc/AjdzOClJO1Uk1nVDh7xwW0rFj2n/BP4VuDkdL1Z8WCV3OzHsM1RTQ6ZiHIe1s++5eG+k/QjyBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T00:47:43.583147Z","bundle_sha256":"83c125f3663f910f1d689667a2b8aaa0b0e47c7abf6f6bf870461b62ad171ee3"}}