{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:EIU5DL7H2WTGRY6J7IHA2ULXGJ","short_pith_number":"pith:EIU5DL7H","schema_version":"1.0","canonical_sha256":"2229d1afe7d5a668e3c9fa0e0d51773265811bb6e64550bec8ece5e4f9566fc5","source":{"kind":"arxiv","id":"hep-th/0511168","version":1},"attestation_state":"computed","paper":{"title":"Potts correlators and the static three-quark potential","license":"","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat"],"primary_cat":"hep-th","authors_text":"G. Delfino, M. Caselle, N. Magnoli, O. Jahn, P. Grinza","submitted_at":"2005-11-16T19:19:21Z","abstract_excerpt":"We discuss the two- and three-point correlators in the two-dimensional three-state Potts model in the high-temperature phase of the model. By using the form factor approach and perturbed conformal field theory methods we are able to describe both the large distance and the short distance behaviours of the correlators. We compare our predictions with a set of high precision Monte-Carlo simulations (performed on the triangular lattice realization of the model) finding a complete agreement in both regimes. In particular we use the two-point correlators to fix the various non-universal constants i"},"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":"hep-th/0511168","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-11-16T19:19:21Z","cross_cats_sorted":["cond-mat.stat-mech","hep-lat"],"title_canon_sha256":"a67c7c20b62883b8be71ccc0e7f566a586d66145fd52de3cd17eb13195fc717d","abstract_canon_sha256":"6c7d76e5f6f82bfb3c6f0b6aa81f5a3e557c4a3f455d2c79eda4345f510e5fd0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:37.365556Z","signature_b64":"fvCJYkNlnO+3rHNOs8OFuVyrOUOg2jTfpVEodGg+MbaQNNgbgsAMGj3mBzDTKMaXjsyjKsaWp64NifW3OkisBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2229d1afe7d5a668e3c9fa0e0d51773265811bb6e64550bec8ece5e4f9566fc5","last_reissued_at":"2026-05-18T04:28:37.365186Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:37.365186Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Potts correlators and the static three-quark potential","license":"","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat"],"primary_cat":"hep-th","authors_text":"G. Delfino, M. Caselle, N. Magnoli, O. Jahn, P. Grinza","submitted_at":"2005-11-16T19:19:21Z","abstract_excerpt":"We discuss the two- and three-point correlators in the two-dimensional three-state Potts model in the high-temperature phase of the model. By using the form factor approach and perturbed conformal field theory methods we are able to describe both the large distance and the short distance behaviours of the correlators. We compare our predictions with a set of high precision Monte-Carlo simulations (performed on the triangular lattice realization of the model) finding a complete agreement in both regimes. In particular we use the two-point correlators to fix the various non-universal constants i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0511168","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0511168","created_at":"2026-05-18T04:28:37.365236+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0511168v1","created_at":"2026-05-18T04:28:37.365236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0511168","created_at":"2026-05-18T04:28:37.365236+00:00"},{"alias_kind":"pith_short_12","alias_value":"EIU5DL7H2WTG","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"EIU5DL7H2WTGRY6J","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"EIU5DL7H","created_at":"2026-05-18T12:25:53.335082+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/EIU5DL7H2WTGRY6J7IHA2ULXGJ","json":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ.json","graph_json":"https://pith.science/api/pith-number/EIU5DL7H2WTGRY6J7IHA2ULXGJ/graph.json","events_json":"https://pith.science/api/pith-number/EIU5DL7H2WTGRY6J7IHA2ULXGJ/events.json","paper":"https://pith.science/paper/EIU5DL7H"},"agent_actions":{"view_html":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ","download_json":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ.json","view_paper":"https://pith.science/paper/EIU5DL7H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0511168&json=true","fetch_graph":"https://pith.science/api/pith-number/EIU5DL7H2WTGRY6J7IHA2ULXGJ/graph.json","fetch_events":"https://pith.science/api/pith-number/EIU5DL7H2WTGRY6J7IHA2ULXGJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ/action/storage_attestation","attest_author":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ/action/author_attestation","sign_citation":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ/action/citation_signature","submit_replication":"https://pith.science/pith/EIU5DL7H2WTGRY6J7IHA2ULXGJ/action/replication_record"}},"created_at":"2026-05-18T04:28:37.365236+00:00","updated_at":"2026-05-18T04:28:37.365236+00:00"}