{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:ORXWAG57WVITM4NQNZQJC4QUVG","short_pith_number":"pith:ORXWAG57","schema_version":"1.0","canonical_sha256":"746f601bbfb5513671b06e60917214a9baf2f58a87574fe649804fa9b77fba19","source":{"kind":"arxiv","id":"1109.0821","version":3},"attestation_state":"computed","paper":{"title":"Evaporation/condensation transition of the two dimensional Potts model in microcanonical ensemble","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Hiroshi Watanabe, Nobuyasu Ito, Tomoaki Nogawa","submitted_at":"2011-09-05T07:59:57Z","abstract_excerpt":"Evaporation/condensation transition of the Potts model on square lattice is numerically investigated by the Wang-Landau sampling method. Intrinsically system size dependent discrete transition between supersaturation state and phase-separation state is observed in the microcanonical ensemble by changing constrained internal energy. We calculate the microcanonical temperature, as a derivative of microcanonical entropy, and condensation ratio, and perform a finite size scaling of them to indicate clear tendency of numerical data to converge to the infinite size limit predicted by phenomenologica"},"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":"1109.0821","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-09-05T07:59:57Z","cross_cats_sorted":[],"title_canon_sha256":"a5f6b0d9014b96fe4b6855b920e9ea9b76c26d9f39d555fc4a8821dc5b665c06","abstract_canon_sha256":"48ca04b527bb9cc9ba69edfae2a3e9a1435e407a43169f7f259a1e8284610e07"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:06:35.494592Z","signature_b64":"WFMDixb0w4HYgb0z+SW4TOCiVETn+955f86w84Tl7TJo9iDWHevTt77wevuVVESCwPYl2SpSytYH0Lr4I7ELAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"746f601bbfb5513671b06e60917214a9baf2f58a87574fe649804fa9b77fba19","last_reissued_at":"2026-05-18T04:06:35.493958Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:06:35.493958Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evaporation/condensation transition of the two dimensional Potts model in microcanonical ensemble","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Hiroshi Watanabe, Nobuyasu Ito, Tomoaki Nogawa","submitted_at":"2011-09-05T07:59:57Z","abstract_excerpt":"Evaporation/condensation transition of the Potts model on square lattice is numerically investigated by the Wang-Landau sampling method. Intrinsically system size dependent discrete transition between supersaturation state and phase-separation state is observed in the microcanonical ensemble by changing constrained internal energy. We calculate the microcanonical temperature, as a derivative of microcanonical entropy, and condensation ratio, and perform a finite size scaling of them to indicate clear tendency of numerical data to converge to the infinite size limit predicted by phenomenologica"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.0821","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1109.0821","created_at":"2026-05-18T04:06:35.494054+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.0821v3","created_at":"2026-05-18T04:06:35.494054+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.0821","created_at":"2026-05-18T04:06:35.494054+00:00"},{"alias_kind":"pith_short_12","alias_value":"ORXWAG57WVIT","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"ORXWAG57WVITM4NQ","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"ORXWAG57","created_at":"2026-05-18T12:26:37.096874+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/ORXWAG57WVITM4NQNZQJC4QUVG","json":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG.json","graph_json":"https://pith.science/api/pith-number/ORXWAG57WVITM4NQNZQJC4QUVG/graph.json","events_json":"https://pith.science/api/pith-number/ORXWAG57WVITM4NQNZQJC4QUVG/events.json","paper":"https://pith.science/paper/ORXWAG57"},"agent_actions":{"view_html":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG","download_json":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG.json","view_paper":"https://pith.science/paper/ORXWAG57","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.0821&json=true","fetch_graph":"https://pith.science/api/pith-number/ORXWAG57WVITM4NQNZQJC4QUVG/graph.json","fetch_events":"https://pith.science/api/pith-number/ORXWAG57WVITM4NQNZQJC4QUVG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG/action/storage_attestation","attest_author":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG/action/author_attestation","sign_citation":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG/action/citation_signature","submit_replication":"https://pith.science/pith/ORXWAG57WVITM4NQNZQJC4QUVG/action/replication_record"}},"created_at":"2026-05-18T04:06:35.494054+00:00","updated_at":"2026-05-18T04:06:35.494054+00:00"}