{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:EKQ3LFFEZM64G5AKB4HSDXR32A","short_pith_number":"pith:EKQ3LFFE","schema_version":"1.0","canonical_sha256":"22a1b594a4cb3dc3740a0f0f21de3bd034cd075c2b4752b0333420cbe4f8f3c4","source":{"kind":"arxiv","id":"hep-lat/0407001","version":1},"attestation_state":"computed","paper":{"title":"First Study for the Pentaquark Potential in SU(3) Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Fumiko Okiharu, Hideo Suganuma, Toru T. Takahashi","submitted_at":"2004-07-02T13:43:32Z","abstract_excerpt":"The static penta-quark (5Q) potential $V_{\\rm 5Q}$ is studied in SU(3) lattice QCD with $16^3\\times 32$ and $\\beta$=6.0 at the quenched level. From the 5Q Wilson loop, $V_{\\rm 5Q}$ is calculated in a gauge-invariant manner, with the smearing method to enhance the ground-state component. $V_{\\rm 5Q}$ is well described by the OGE plus multi-Y Ansatz: a sum of the OGE Coulomb term and the multi-Y-type linear term proportional to the minimal total length of the flux-tube linking the five quarks. Comparing with ${\\rm Q \\bar Q}$ and 3Q potentials, we find a universality of the string tension, $\\sigm"},"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/0407001","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-07-02T13:43:32Z","cross_cats_sorted":[],"title_canon_sha256":"ca9e211107b17cf05db30d0dd2e9667c6f060b5b1bdcb724d5e92f8a3d55dcc7","abstract_canon_sha256":"ea368b6f1ffa5c066984b58e10370bf4cd767eab4d2857889adb4789a39d8d5d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:48:00.772858Z","signature_b64":"GzOjVSxYTNS87H8Fcp/P+f9IanckKELDHMkIbWTU705eHqH7Gj1oueyQMKV8umF3X9VSIrVSS10VQ/9o91DJCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22a1b594a4cb3dc3740a0f0f21de3bd034cd075c2b4752b0333420cbe4f8f3c4","last_reissued_at":"2026-07-04T16:48:00.772479Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:48:00.772479Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First Study for the Pentaquark Potential in SU(3) Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Fumiko Okiharu, Hideo Suganuma, Toru T. Takahashi","submitted_at":"2004-07-02T13:43:32Z","abstract_excerpt":"The static penta-quark (5Q) potential $V_{\\rm 5Q}$ is studied in SU(3) lattice QCD with $16^3\\times 32$ and $\\beta$=6.0 at the quenched level. From the 5Q Wilson loop, $V_{\\rm 5Q}$ is calculated in a gauge-invariant manner, with the smearing method to enhance the ground-state component. $V_{\\rm 5Q}$ is well described by the OGE plus multi-Y Ansatz: a sum of the OGE Coulomb term and the multi-Y-type linear term proportional to the minimal total length of the flux-tube linking the five quarks. Comparing with ${\\rm Q \\bar Q}$ and 3Q potentials, we find a universality of the string tension, $\\sigm"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0407001","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/0407001/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/0407001","created_at":"2026-07-04T16:48:00.772535+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0407001v1","created_at":"2026-07-04T16:48:00.772535+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0407001","created_at":"2026-07-04T16:48:00.772535+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKQ3LFFEZM64","created_at":"2026-07-04T16:48:00.772535+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKQ3LFFEZM64G5AK","created_at":"2026-07-04T16:48:00.772535+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKQ3LFFE","created_at":"2026-07-04T16:48:00.772535+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.10164","citing_title":"Cluster reducibility of multiquark operators","ref_index":42,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A","json":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A.json","graph_json":"https://pith.science/api/pith-number/EKQ3LFFEZM64G5AKB4HSDXR32A/graph.json","events_json":"https://pith.science/api/pith-number/EKQ3LFFEZM64G5AKB4HSDXR32A/events.json","paper":"https://pith.science/paper/EKQ3LFFE"},"agent_actions":{"view_html":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A","download_json":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A.json","view_paper":"https://pith.science/paper/EKQ3LFFE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0407001&json=true","fetch_graph":"https://pith.science/api/pith-number/EKQ3LFFEZM64G5AKB4HSDXR32A/graph.json","fetch_events":"https://pith.science/api/pith-number/EKQ3LFFEZM64G5AKB4HSDXR32A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A/action/storage_attestation","attest_author":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A/action/author_attestation","sign_citation":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A/action/citation_signature","submit_replication":"https://pith.science/pith/EKQ3LFFEZM64G5AKB4HSDXR32A/action/replication_record"}},"created_at":"2026-07-04T16:48:00.772535+00:00","updated_at":"2026-07-04T16:48:00.772535+00:00"}