{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:WVWXUSLT3CQN4AKQCMBZJPV2LO","short_pith_number":"pith:WVWXUSLT","schema_version":"1.0","canonical_sha256":"b56d7a4973d8a0de0150130394beba5b9878300b6fa5d7e0ca2b21ae023da75b","source":{"kind":"arxiv","id":"1609.02869","version":2},"attestation_state":"computed","paper":{"title":"Finite size scaling analysis of a nonequilibrium phase transition in the naming game model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.comp-ph"],"primary_cat":"physics.soc-ph","authors_text":"A. Hern\\'andez, E. Brigatti","submitted_at":"2016-09-09T17:32:06Z","abstract_excerpt":"We realize an extensive numerical study of the Naming Game model with a noise term which accounts for perturbations. This model displays a non-equilibrium phase transition between an absorbing ordered consensus state, which occurs for small noise, and a disordered phase with fragmented clusters characterized by heterogeneous memories, which emerges at strong noise levels. The nature of the phase transition is studied by means of a finite-size scaling analysis of the moments. We observe a scaling behavior typical of a discontinuous transition and we are able to estimate the thermodynamic limit."},"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":"1609.02869","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2016-09-09T17:32:06Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"f98d25bfefaee860cebd9e98d4d99d90e6941a6f8e9d57fe207bb34b2c676a04","abstract_canon_sha256":"cc13ba37c06d5f280664597721cb8f42f55a0a94626dc07fc821dfb44ba3a138"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:59:19.332134Z","signature_b64":"DbKvDeY6hlEx2gOWCiHg/lCTvCD0oPyEg3X0SEnxS85CwjiXUttPUL6LY3e/mFqWP8TjZhdaAdiZiqgmyB82CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b56d7a4973d8a0de0150130394beba5b9878300b6fa5d7e0ca2b21ae023da75b","last_reissued_at":"2026-05-18T00:59:19.331332Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:59:19.331332Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite size scaling analysis of a nonequilibrium phase transition in the naming game model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.comp-ph"],"primary_cat":"physics.soc-ph","authors_text":"A. Hern\\'andez, E. Brigatti","submitted_at":"2016-09-09T17:32:06Z","abstract_excerpt":"We realize an extensive numerical study of the Naming Game model with a noise term which accounts for perturbations. This model displays a non-equilibrium phase transition between an absorbing ordered consensus state, which occurs for small noise, and a disordered phase with fragmented clusters characterized by heterogeneous memories, which emerges at strong noise levels. The nature of the phase transition is studied by means of a finite-size scaling analysis of the moments. We observe a scaling behavior typical of a discontinuous transition and we are able to estimate the thermodynamic limit."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.02869","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":"1609.02869","created_at":"2026-05-18T00:59:19.331465+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.02869v2","created_at":"2026-05-18T00:59:19.331465+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.02869","created_at":"2026-05-18T00:59:19.331465+00:00"},{"alias_kind":"pith_short_12","alias_value":"WVWXUSLT3CQN","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_16","alias_value":"WVWXUSLT3CQN4AKQ","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_8","alias_value":"WVWXUSLT","created_at":"2026-05-18T12:30:51.357362+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/WVWXUSLT3CQN4AKQCMBZJPV2LO","json":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO.json","graph_json":"https://pith.science/api/pith-number/WVWXUSLT3CQN4AKQCMBZJPV2LO/graph.json","events_json":"https://pith.science/api/pith-number/WVWXUSLT3CQN4AKQCMBZJPV2LO/events.json","paper":"https://pith.science/paper/WVWXUSLT"},"agent_actions":{"view_html":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO","download_json":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO.json","view_paper":"https://pith.science/paper/WVWXUSLT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.02869&json=true","fetch_graph":"https://pith.science/api/pith-number/WVWXUSLT3CQN4AKQCMBZJPV2LO/graph.json","fetch_events":"https://pith.science/api/pith-number/WVWXUSLT3CQN4AKQCMBZJPV2LO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO/action/storage_attestation","attest_author":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO/action/author_attestation","sign_citation":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO/action/citation_signature","submit_replication":"https://pith.science/pith/WVWXUSLT3CQN4AKQCMBZJPV2LO/action/replication_record"}},"created_at":"2026-05-18T00:59:19.331465+00:00","updated_at":"2026-05-18T00:59:19.331465+00:00"}