{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:FAENTF2LH43TC5JPZVSSSDPNCM","short_pith_number":"pith:FAENTF2L","canonical_record":{"source":{"id":"1608.07091","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-08-25T11:36:05Z","cross_cats_sorted":[],"title_canon_sha256":"b829cfa6984fc1bc7c4d0c468322e709a92b9962afba7d5db9330c4b47bee038","abstract_canon_sha256":"5933b2a088239af6b0c2d4a77a89f14da17023d48975b4bc5d7d331982f4deac"},"schema_version":"1.0"},"canonical_sha256":"2808d9974b3f3731752fcd65290ded1307216d0cac901270de9debe6d152303b","source":{"kind":"arxiv","id":"1608.07091","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.07091","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"arxiv_version","alias_value":"1608.07091v1","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07091","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"pith_short_12","alias_value":"FAENTF2LH43T","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FAENTF2LH43TC5JP","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FAENTF2L","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:FAENTF2LH43TC5JPZVSSSDPNCM","target":"record","payload":{"canonical_record":{"source":{"id":"1608.07091","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-08-25T11:36:05Z","cross_cats_sorted":[],"title_canon_sha256":"b829cfa6984fc1bc7c4d0c468322e709a92b9962afba7d5db9330c4b47bee038","abstract_canon_sha256":"5933b2a088239af6b0c2d4a77a89f14da17023d48975b4bc5d7d331982f4deac"},"schema_version":"1.0"},"canonical_sha256":"2808d9974b3f3731752fcd65290ded1307216d0cac901270de9debe6d152303b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:33.427989Z","signature_b64":"ND2smOD0TBMXzRK4Z7SXoGjReaDxnNPLoTr+zy4+ifBTwklO9nWktOmL7fLBuM65Paxs33r6LBINn2lSO7syBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2808d9974b3f3731752fcd65290ded1307216d0cac901270de9debe6d152303b","last_reissued_at":"2026-05-18T00:40:33.427331Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:33.427331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.07091","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:40:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ks6XLMB3wFzaCB9Vb5lv64pCOI3Dlylz8YQXOqTOKNQlLlMHcoWiK9YSnpLVjPopuXdpwBK/N4qt+CEMtT2qCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T12:46:24.665836Z"},"content_sha256":"8362b3f5a9bb23fbf943f616fb2e8c9d371f1f7e5dac2c01ebf4479b87b34765","schema_version":"1.0","event_id":"sha256:8362b3f5a9bb23fbf943f616fb2e8c9d371f1f7e5dac2c01ebf4479b87b34765"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:FAENTF2LH43TC5JPZVSSSDPNCM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exact solution of the isotropic majority-vote model on complete graphs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Agata Fronczak, Piotr Fronczak","submitted_at":"2016-08-25T11:36:05Z","abstract_excerpt":"The isotropic majority-vote (MV) model which, apart from the one-dimensional case, is thought to be non-equilibrium and violating the detailed balance condition. We show that this is not true, when the model is defined on a complete graph. In the stationary regime, the MV model on a fully connected graph fulfills the detailed balance. We derive the exact expression for the probability distribution of finding the system in a given spin configuration. We show that it only depends on the absolute value of magnetization. Our theoretical predictions are validated by numerical simulations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07091","kind":"arxiv","version":1},"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":"2026-05-18T00:40:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3XGgDHFxXlmOQLxG+hlIjJY657Z5/ICtEexcckICwod81XDDD9f6cqRj8MhHy+KU7w3Z0aWvVoL3eBOtij6YDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T12:46:24.666177Z"},"content_sha256":"ca8b1e10a0573b377c494494bb86ca3df0bf3b50384ed93d447cf7cd9c3af9bd","schema_version":"1.0","event_id":"sha256:ca8b1e10a0573b377c494494bb86ca3df0bf3b50384ed93d447cf7cd9c3af9bd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FAENTF2LH43TC5JPZVSSSDPNCM/bundle.json","state_url":"https://pith.science/pith/FAENTF2LH43TC5JPZVSSSDPNCM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FAENTF2LH43TC5JPZVSSSDPNCM/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":"2026-05-28T12:46:24Z","links":{"resolver":"https://pith.science/pith/FAENTF2LH43TC5JPZVSSSDPNCM","bundle":"https://pith.science/pith/FAENTF2LH43TC5JPZVSSSDPNCM/bundle.json","state":"https://pith.science/pith/FAENTF2LH43TC5JPZVSSSDPNCM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FAENTF2LH43TC5JPZVSSSDPNCM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FAENTF2LH43TC5JPZVSSSDPNCM","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":"5933b2a088239af6b0c2d4a77a89f14da17023d48975b4bc5d7d331982f4deac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-08-25T11:36:05Z","title_canon_sha256":"b829cfa6984fc1bc7c4d0c468322e709a92b9962afba7d5db9330c4b47bee038"},"schema_version":"1.0","source":{"id":"1608.07091","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.07091","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"arxiv_version","alias_value":"1608.07091v1","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07091","created_at":"2026-05-18T00:40:33Z"},{"alias_kind":"pith_short_12","alias_value":"FAENTF2LH43T","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FAENTF2LH43TC5JP","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FAENTF2L","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:ca8b1e10a0573b377c494494bb86ca3df0bf3b50384ed93d447cf7cd9c3af9bd","target":"graph","created_at":"2026-05-18T00:40:33Z","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 isotropic majority-vote (MV) model which, apart from the one-dimensional case, is thought to be non-equilibrium and violating the detailed balance condition. We show that this is not true, when the model is defined on a complete graph. In the stationary regime, the MV model on a fully connected graph fulfills the detailed balance. We derive the exact expression for the probability distribution of finding the system in a given spin configuration. We show that it only depends on the absolute value of magnetization. Our theoretical predictions are validated by numerical simulations.","authors_text":"Agata Fronczak, Piotr Fronczak","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-08-25T11:36:05Z","title":"Exact solution of the isotropic majority-vote model on complete graphs"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07091","kind":"arxiv","version":1},"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":"sha256:8362b3f5a9bb23fbf943f616fb2e8c9d371f1f7e5dac2c01ebf4479b87b34765","target":"record","created_at":"2026-05-18T00:40:33Z","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":"5933b2a088239af6b0c2d4a77a89f14da17023d48975b4bc5d7d331982f4deac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-08-25T11:36:05Z","title_canon_sha256":"b829cfa6984fc1bc7c4d0c468322e709a92b9962afba7d5db9330c4b47bee038"},"schema_version":"1.0","source":{"id":"1608.07091","kind":"arxiv","version":1}},"canonical_sha256":"2808d9974b3f3731752fcd65290ded1307216d0cac901270de9debe6d152303b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2808d9974b3f3731752fcd65290ded1307216d0cac901270de9debe6d152303b","first_computed_at":"2026-05-18T00:40:33.427331Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:33.427331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ND2smOD0TBMXzRK4Z7SXoGjReaDxnNPLoTr+zy4+ifBTwklO9nWktOmL7fLBuM65Paxs33r6LBINn2lSO7syBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:33.427989Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.07091","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8362b3f5a9bb23fbf943f616fb2e8c9d371f1f7e5dac2c01ebf4479b87b34765","sha256:ca8b1e10a0573b377c494494bb86ca3df0bf3b50384ed93d447cf7cd9c3af9bd"],"state_sha256":"8b251d08b34f5a86682c9203a0bf34106d6ec8bc7f20530ba4b6ba413f2406dc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uhtCL2BaQZafn/MPikB3kijZY3cDb8IGFN8ty8Xj0jEqV8qZFnVZo8uVoYwDNp2iUqsr9yIOtdj+7033P/8sDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T12:46:24.668122Z","bundle_sha256":"eaacf2d20e26cce5a828231fa71abb915467e0d289ea13798baa4350eaeca810"}}