{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:5VS4PLZAVHZS7ZUAFKOGIGOLRC","short_pith_number":"pith:5VS4PLZA","canonical_record":{"source":{"id":"1605.05161","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-05-17T13:39:52Z","cross_cats_sorted":["physics.bio-ph","q-bio.QM"],"title_canon_sha256":"bd0f8bdaf4dda155585a693fa1356eec58ae6f875177c278450445c0243ecd3a","abstract_canon_sha256":"e3c15e6718e847d6d70210e0c7e5610f71dd154fbf1eb19fda5781ac028558e1"},"schema_version":"1.0"},"canonical_sha256":"ed65c7af20a9f32fe6802a9c6419cb889d0587a1bf9bd2a751fc8b5606dfd51e","source":{"kind":"arxiv","id":"1605.05161","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05161","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05161v2","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05161","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"pith_short_12","alias_value":"5VS4PLZAVHZS","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5VS4PLZAVHZS7ZUA","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5VS4PLZA","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:5VS4PLZAVHZS7ZUAFKOGIGOLRC","target":"record","payload":{"canonical_record":{"source":{"id":"1605.05161","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-05-17T13:39:52Z","cross_cats_sorted":["physics.bio-ph","q-bio.QM"],"title_canon_sha256":"bd0f8bdaf4dda155585a693fa1356eec58ae6f875177c278450445c0243ecd3a","abstract_canon_sha256":"e3c15e6718e847d6d70210e0c7e5610f71dd154fbf1eb19fda5781ac028558e1"},"schema_version":"1.0"},"canonical_sha256":"ed65c7af20a9f32fe6802a9c6419cb889d0587a1bf9bd2a751fc8b5606dfd51e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:03.465287Z","signature_b64":"pjs2xHakvlMK3V4hd9jtSnrEbMwGurLEoxybXF7psrzQQMzn6P1xwJnpVRs5WG0PmeFQ6kpresFoXNi4u98iCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed65c7af20a9f32fe6802a9c6419cb889d0587a1bf9bd2a751fc8b5606dfd51e","last_reissued_at":"2026-05-18T01:12:03.464858Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:03.464858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.05161","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":"2026-05-18T01:12:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k8tBXdnv4OxBGsFWj+2D9HUIweo8xSRmI2PbLyAg4u+nUTtz/A66QDvs4dpglZ+7RD14lw7d5f0a9PBcuBPXCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:30:23.684759Z"},"content_sha256":"1d8bb7c7fa65efbf8e22267a1f51ba55e07d0024a335cdc19ac1e68adf617b03","schema_version":"1.0","event_id":"sha256:1d8bb7c7fa65efbf8e22267a1f51ba55e07d0024a335cdc19ac1e68adf617b03"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:5VS4PLZAVHZS7ZUAFKOGIGOLRC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Self-Organized Bistability Associated With First-Order Phase Transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.bio-ph","q-bio.QM"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alessandro Vezzani, Miguel A. Mu\\~noz, Raffaella Burioni, Serena Di Santo","submitted_at":"2016-05-17T13:39:52Z","abstract_excerpt":"Self-organized criticality elucidates the conditions under which physical and biological systems tune themselves to the edge of a second-order phase transition, with scale invariance. Motivated by the empirical observation of bimodal distributions of activity in neuroscience and other fields, we propose and analyze a theory for the self-organization to the point of phase-coexistence in systems exhibiting a first-order phase transition. It explains the emergence of regular avalanches with attributes of scale-invariance which coexist with huge anomalous ones, with realizations in many fields."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05161","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":"2026-05-18T01:12:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OUX8b4ZRFH2rq+wCueMuVZjjzHf1QhX8Dnk2mgb6AKghnboAIIZ6mlr3ISfGB05C9rpksVluLGs4A8iE0z8LDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:30:23.685236Z"},"content_sha256":"b3294f4ffce7d4419c1d2eba60c6dc039d9ee2673bfb449f3f37d7dd43a33382","schema_version":"1.0","event_id":"sha256:b3294f4ffce7d4419c1d2eba60c6dc039d9ee2673bfb449f3f37d7dd43a33382"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/bundle.json","state_url":"https://pith.science/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/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":"2026-06-02T07:30:23Z","links":{"resolver":"https://pith.science/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC","bundle":"https://pith.science/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/bundle.json","state":"https://pith.science/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5VS4PLZAVHZS7ZUAFKOGIGOLRC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5VS4PLZAVHZS7ZUAFKOGIGOLRC","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":"e3c15e6718e847d6d70210e0c7e5610f71dd154fbf1eb19fda5781ac028558e1","cross_cats_sorted":["physics.bio-ph","q-bio.QM"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-05-17T13:39:52Z","title_canon_sha256":"bd0f8bdaf4dda155585a693fa1356eec58ae6f875177c278450445c0243ecd3a"},"schema_version":"1.0","source":{"id":"1605.05161","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05161","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05161v2","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05161","created_at":"2026-05-18T01:12:03Z"},{"alias_kind":"pith_short_12","alias_value":"5VS4PLZAVHZS","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5VS4PLZAVHZS7ZUA","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5VS4PLZA","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:b3294f4ffce7d4419c1d2eba60c6dc039d9ee2673bfb449f3f37d7dd43a33382","target":"graph","created_at":"2026-05-18T01:12:03Z","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":"Self-organized criticality elucidates the conditions under which physical and biological systems tune themselves to the edge of a second-order phase transition, with scale invariance. Motivated by the empirical observation of bimodal distributions of activity in neuroscience and other fields, we propose and analyze a theory for the self-organization to the point of phase-coexistence in systems exhibiting a first-order phase transition. It explains the emergence of regular avalanches with attributes of scale-invariance which coexist with huge anomalous ones, with realizations in many fields.","authors_text":"Alessandro Vezzani, Miguel A. Mu\\~noz, Raffaella Burioni, Serena Di Santo","cross_cats":["physics.bio-ph","q-bio.QM"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-05-17T13:39:52Z","title":"Self-Organized Bistability Associated With First-Order Phase Transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05161","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":"sha256:1d8bb7c7fa65efbf8e22267a1f51ba55e07d0024a335cdc19ac1e68adf617b03","target":"record","created_at":"2026-05-18T01:12:03Z","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":"e3c15e6718e847d6d70210e0c7e5610f71dd154fbf1eb19fda5781ac028558e1","cross_cats_sorted":["physics.bio-ph","q-bio.QM"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-05-17T13:39:52Z","title_canon_sha256":"bd0f8bdaf4dda155585a693fa1356eec58ae6f875177c278450445c0243ecd3a"},"schema_version":"1.0","source":{"id":"1605.05161","kind":"arxiv","version":2}},"canonical_sha256":"ed65c7af20a9f32fe6802a9c6419cb889d0587a1bf9bd2a751fc8b5606dfd51e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ed65c7af20a9f32fe6802a9c6419cb889d0587a1bf9bd2a751fc8b5606dfd51e","first_computed_at":"2026-05-18T01:12:03.464858Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:03.464858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pjs2xHakvlMK3V4hd9jtSnrEbMwGurLEoxybXF7psrzQQMzn6P1xwJnpVRs5WG0PmeFQ6kpresFoXNi4u98iCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:03.465287Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.05161","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1d8bb7c7fa65efbf8e22267a1f51ba55e07d0024a335cdc19ac1e68adf617b03","sha256:b3294f4ffce7d4419c1d2eba60c6dc039d9ee2673bfb449f3f37d7dd43a33382"],"state_sha256":"8bfcec64fbb35050557e25ca0dc703ad1a67c3a75792907ded1a407c0776891c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z72pIkW5RNplnJ3gZ32gL3JmQoN2IOfstWp6OcoSzbIjR4eFD0YNUWuLSfO/G6P+RqGcRcTw2JE7psxf+anNBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T07:30:23.687809Z","bundle_sha256":"eae8373b0e0db0ed86490ed58137c7988e681634ff65c25c9f5444956067cba5"}}