{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:6YNWPKM5PET5A4TFOS6LP64PQX","short_pith_number":"pith:6YNWPKM5","canonical_record":{"source":{"id":"1701.09184","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-31T18:55:11Z","cross_cats_sorted":[],"title_canon_sha256":"ade4acb0d4b93de3e89d33e03c3fd2f01ac45b2510c94c23561db2fb163d2e38","abstract_canon_sha256":"a05e420e8cc7c01586f365cdf8a0da2a6520031b357df5f27ecba314d5484882"},"schema_version":"1.0"},"canonical_sha256":"f61b67a99d7927d0726574bcb7fb8f85da414c148cc3c5a652998dd331f16f12","source":{"kind":"arxiv","id":"1701.09184","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.09184","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"arxiv_version","alias_value":"1701.09184v3","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.09184","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"pith_short_12","alias_value":"6YNWPKM5PET5","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6YNWPKM5PET5A4TF","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6YNWPKM5","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:6YNWPKM5PET5A4TFOS6LP64PQX","target":"record","payload":{"canonical_record":{"source":{"id":"1701.09184","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-31T18:55:11Z","cross_cats_sorted":[],"title_canon_sha256":"ade4acb0d4b93de3e89d33e03c3fd2f01ac45b2510c94c23561db2fb163d2e38","abstract_canon_sha256":"a05e420e8cc7c01586f365cdf8a0da2a6520031b357df5f27ecba314d5484882"},"schema_version":"1.0"},"canonical_sha256":"f61b67a99d7927d0726574bcb7fb8f85da414c148cc3c5a652998dd331f16f12","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:25.067786Z","signature_b64":"/YsBpCtOqIvzjG2+2lqdyG7MPRDaFrrmNL3kL3Njsd/NuGqj7zzyZMl/9Hqnj+C065NX+TwHh0eL9K6LdtyUAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f61b67a99d7927d0726574bcb7fb8f85da414c148cc3c5a652998dd331f16f12","last_reissued_at":"2026-05-18T00:41:25.067149Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:25.067149Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1701.09184","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:41:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vGXgU5bC48SCaC/RVsu2CUDjYPquwyVgsKJhOq5qZ5BV9b8c1GzIAg8OzxDrghcvRwf6UkXNeULYfDmHxiqgAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T14:14:14.441406Z"},"content_sha256":"ac90f121431b5213f6a26cd63ac6647bd8baaa2af1e9440fe7f588d152d0a61a","schema_version":"1.0","event_id":"sha256:ac90f121431b5213f6a26cd63ac6647bd8baaa2af1e9440fe7f588d152d0a61a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:6YNWPKM5PET5A4TFOS6LP64PQX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effects of diffusion in competitive contact processes on bipartite lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"C. E. Fiore, M. M. de Oliveira","submitted_at":"2017-01-31T18:55:11Z","abstract_excerpt":"We investigate the influence of particle diffusion in the two-dimension contact process (CP) with a competitive dynamics in bipartite sublattices, proposed in [Phys. Rev. E 84, 011125 (2011)]. The particle creation depends on its first and second neighbors and the extinction increases according to the local density. In contrast to the standard CP model, mean-field theory and numerical simulations predict three stable phases: inactive (absorbing), active symmetric and active asymmetric, signed by distinct sublattice particle occupations. Our results from MFT and Monte Carlo simulations reveal t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.09184","kind":"arxiv","version":3},"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":"2026-05-18T00:41:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pcHfLOv66iovi2lHQEBp87rDu0WQMvAxdDPYANpU7CfJ7/zyt46VdSRJqCjjcveVw4qq54JEvm2uSYQm6iSICA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T14:14:14.441765Z"},"content_sha256":"534ad891bced5f2ef3f84bfc8a8754e67c75689973b77e531c418b1927a8978f","schema_version":"1.0","event_id":"sha256:534ad891bced5f2ef3f84bfc8a8754e67c75689973b77e531c418b1927a8978f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6YNWPKM5PET5A4TFOS6LP64PQX/bundle.json","state_url":"https://pith.science/pith/6YNWPKM5PET5A4TFOS6LP64PQX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6YNWPKM5PET5A4TFOS6LP64PQX/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":"2026-06-22T14:14:14Z","links":{"resolver":"https://pith.science/pith/6YNWPKM5PET5A4TFOS6LP64PQX","bundle":"https://pith.science/pith/6YNWPKM5PET5A4TFOS6LP64PQX/bundle.json","state":"https://pith.science/pith/6YNWPKM5PET5A4TFOS6LP64PQX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6YNWPKM5PET5A4TFOS6LP64PQX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:6YNWPKM5PET5A4TFOS6LP64PQX","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":"a05e420e8cc7c01586f365cdf8a0da2a6520031b357df5f27ecba314d5484882","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-31T18:55:11Z","title_canon_sha256":"ade4acb0d4b93de3e89d33e03c3fd2f01ac45b2510c94c23561db2fb163d2e38"},"schema_version":"1.0","source":{"id":"1701.09184","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.09184","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"arxiv_version","alias_value":"1701.09184v3","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.09184","created_at":"2026-05-18T00:41:25Z"},{"alias_kind":"pith_short_12","alias_value":"6YNWPKM5PET5","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6YNWPKM5PET5A4TF","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6YNWPKM5","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:534ad891bced5f2ef3f84bfc8a8754e67c75689973b77e531c418b1927a8978f","target":"graph","created_at":"2026-05-18T00:41:25Z","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":"We investigate the influence of particle diffusion in the two-dimension contact process (CP) with a competitive dynamics in bipartite sublattices, proposed in [Phys. Rev. E 84, 011125 (2011)]. The particle creation depends on its first and second neighbors and the extinction increases according to the local density. In contrast to the standard CP model, mean-field theory and numerical simulations predict three stable phases: inactive (absorbing), active symmetric and active asymmetric, signed by distinct sublattice particle occupations. Our results from MFT and Monte Carlo simulations reveal t","authors_text":"C. E. Fiore, M. M. de Oliveira","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-31T18:55:11Z","title":"Effects of diffusion in competitive contact processes on bipartite lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.09184","kind":"arxiv","version":3},"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:ac90f121431b5213f6a26cd63ac6647bd8baaa2af1e9440fe7f588d152d0a61a","target":"record","created_at":"2026-05-18T00:41:25Z","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":"a05e420e8cc7c01586f365cdf8a0da2a6520031b357df5f27ecba314d5484882","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-31T18:55:11Z","title_canon_sha256":"ade4acb0d4b93de3e89d33e03c3fd2f01ac45b2510c94c23561db2fb163d2e38"},"schema_version":"1.0","source":{"id":"1701.09184","kind":"arxiv","version":3}},"canonical_sha256":"f61b67a99d7927d0726574bcb7fb8f85da414c148cc3c5a652998dd331f16f12","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f61b67a99d7927d0726574bcb7fb8f85da414c148cc3c5a652998dd331f16f12","first_computed_at":"2026-05-18T00:41:25.067149Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:41:25.067149Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/YsBpCtOqIvzjG2+2lqdyG7MPRDaFrrmNL3kL3Njsd/NuGqj7zzyZMl/9Hqnj+C065NX+TwHh0eL9K6LdtyUAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:41:25.067786Z","signed_message":"canonical_sha256_bytes"},"source_id":"1701.09184","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ac90f121431b5213f6a26cd63ac6647bd8baaa2af1e9440fe7f588d152d0a61a","sha256:534ad891bced5f2ef3f84bfc8a8754e67c75689973b77e531c418b1927a8978f"],"state_sha256":"6e42c18cbcc04313010904b65ebfab8fbee613a638261678d34ca74d79c58db1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yAKN6XmPMIZJH0Wc09CXD7liqkO8va7FxSd6wddzd9Lc9VGgQW3VY/iA/kPYuXMwDbr/sQX/tLQRmMZ6/XpTAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T14:14:14.443769Z","bundle_sha256":"4e4e03ea0f805b9d3f8a7b6d151b3e33fc51585deefb57e5ca38b7cce4999c85"}}