{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:4FCH6KMKNOMOBU77C3V4OSVITG","short_pith_number":"pith:4FCH6KMK","schema_version":"1.0","canonical_sha256":"e1447f298a6b98e0d3ff16ebc74aa899bdec6bf2b23e9fbbbc5f4a0af376256a","source":{"kind":"arxiv","id":"hep-lat/0204011","version":1},"attestation_state":"computed","paper":{"title":"Detailed Analysis of the Three Quark Potential in SU(3) Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Matsufuru, H. Suganuma, T.T. Takahashi, Y. Nemoto","submitted_at":"2002-04-10T07:37:28Z","abstract_excerpt":"The static three-quark (3Q) potential is studied in detail using SU(3) lattice QCD with $12^3 \\times 24$ at $\\beta=5.7$ and $16^3 \\times 32$ at $\\beta=5.8$, 6.0 at the quenched level. For more than 300 different patterns of the 3Q systems, we perform the accurate measurement of the 3Q Wilson loop with the smearing method, which reduces excited-state contaminations, and present the lattice QCD data of the 3Q ground-state potential $V_{\\rm 3Q}$. We perform the detailed fit analysis on $V_{\\rm 3Q}$ in terms of the Y-ansatz both with the continuum Coulomb potential and with the lattice Coulomb pot"},"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-lat/0204011","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2002-04-10T07:37:28Z","cross_cats_sorted":[],"title_canon_sha256":"61c4903bf0b27c3e49dca506490b3e17ed345fd65205fd7a4eb87a07960c2949","abstract_canon_sha256":"8d7a5b2c11aa1a402a51415cee2d80c743acf2d923860f3c8aeed63118f85522"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:33:52.828909Z","signature_b64":"poE72mlsFBVx7IPYL40dm8+mi/1lSbpfyMUdakf0X3Z9AJqK/4PaiwEYQ4EHnDZdSVlkRKr/LFZexzXf3QZ/Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1447f298a6b98e0d3ff16ebc74aa899bdec6bf2b23e9fbbbc5f4a0af376256a","last_reissued_at":"2026-07-04T16:33:52.828550Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:33:52.828550Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Detailed Analysis of the Three Quark Potential in SU(3) Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"H. Matsufuru, H. Suganuma, T.T. Takahashi, Y. Nemoto","submitted_at":"2002-04-10T07:37:28Z","abstract_excerpt":"The static three-quark (3Q) potential is studied in detail using SU(3) lattice QCD with $12^3 \\times 24$ at $\\beta=5.7$ and $16^3 \\times 32$ at $\\beta=5.8$, 6.0 at the quenched level. For more than 300 different patterns of the 3Q systems, we perform the accurate measurement of the 3Q Wilson loop with the smearing method, which reduces excited-state contaminations, and present the lattice QCD data of the 3Q ground-state potential $V_{\\rm 3Q}$. We perform the detailed fit analysis on $V_{\\rm 3Q}$ in terms of the Y-ansatz both with the continuum Coulomb potential and with the lattice Coulomb pot"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0204011","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/0204011/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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-lat/0204011","created_at":"2026-07-04T16:33:52.828611+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0204011v1","created_at":"2026-07-04T16:33:52.828611+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0204011","created_at":"2026-07-04T16:33:52.828611+00:00"},{"alias_kind":"pith_short_12","alias_value":"4FCH6KMKNOMO","created_at":"2026-07-04T16:33:52.828611+00:00"},{"alias_kind":"pith_short_16","alias_value":"4FCH6KMKNOMOBU77","created_at":"2026-07-04T16:33:52.828611+00:00"},{"alias_kind":"pith_short_8","alias_value":"4FCH6KMK","created_at":"2026-07-04T16:33:52.828611+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.21755","citing_title":"Universalities of Defects in Quantum Field Theories","ref_index":136,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG","json":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG.json","graph_json":"https://pith.science/api/pith-number/4FCH6KMKNOMOBU77C3V4OSVITG/graph.json","events_json":"https://pith.science/api/pith-number/4FCH6KMKNOMOBU77C3V4OSVITG/events.json","paper":"https://pith.science/paper/4FCH6KMK"},"agent_actions":{"view_html":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG","download_json":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG.json","view_paper":"https://pith.science/paper/4FCH6KMK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0204011&json=true","fetch_graph":"https://pith.science/api/pith-number/4FCH6KMKNOMOBU77C3V4OSVITG/graph.json","fetch_events":"https://pith.science/api/pith-number/4FCH6KMKNOMOBU77C3V4OSVITG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG/action/storage_attestation","attest_author":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG/action/author_attestation","sign_citation":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG/action/citation_signature","submit_replication":"https://pith.science/pith/4FCH6KMKNOMOBU77C3V4OSVITG/action/replication_record"}},"created_at":"2026-07-04T16:33:52.828611+00:00","updated_at":"2026-07-04T16:33:52.828611+00:00"}