{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1992:EKXUNVTFDHSK4VMFPUOTCDO4YN","short_pith_number":"pith:EKXUNVTF","schema_version":"1.0","canonical_sha256":"22af46d66519e4ae55857d1d310ddcc379a743408ef12771b2a0326ad5a461ef","source":{"kind":"arxiv","id":"hep-lat/9209008","version":1},"attestation_state":"computed","paper":{"title":"The Running Coupling from SU(3) Lattice Gauge Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A.C. Irving, A. Hulsebos, C. Michael, D.S. Henty, P.W. Stephenson, The UKQCD Collaboration: S.P. Booth","submitted_at":"1992-09-03T18:04:45Z","abstract_excerpt":"{}From an accurate determination of the inter-quark potential, one can study the running coupling constant for a range of $R$-values and hence estimate the scale $\\Lambda_{\\msbar} $. Detailed results are presented for $SU(3)$ pure gauge theory."},"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/9209008","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1992-09-03T18:04:45Z","cross_cats_sorted":[],"title_canon_sha256":"c617f988422848198dcea590af074d7be33745d16ff591581b55048fa712add4","abstract_canon_sha256":"5b7e0bfd5a1dffa42cb689dfb1ec28b080c6551600839e5d5519a1f31385466f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:28.190685Z","signature_b64":"Xuo/Zo8M57PIrQEgfUe8TQAa8I8GzW5CZ5DAMiAo7TE9ewugeDXJVFncVjCsXqWgNPw7X3ysWuJY5YLzjT3xAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22af46d66519e4ae55857d1d310ddcc379a743408ef12771b2a0326ad5a461ef","last_reissued_at":"2026-05-18T04:28:28.190242Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:28.190242Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Running Coupling from SU(3) Lattice Gauge Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A.C. Irving, A. Hulsebos, C. Michael, D.S. Henty, P.W. Stephenson, The UKQCD Collaboration: S.P. Booth","submitted_at":"1992-09-03T18:04:45Z","abstract_excerpt":"{}From an accurate determination of the inter-quark potential, one can study the running coupling constant for a range of $R$-values and hence estimate the scale $\\Lambda_{\\msbar} $. Detailed results are presented for $SU(3)$ pure gauge theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9209008","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-lat/9209008","created_at":"2026-05-18T04:28:28.190324+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9209008v1","created_at":"2026-05-18T04:28:28.190324+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9209008","created_at":"2026-05-18T04:28:28.190324+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKXUNVTFDHSK","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKXUNVTFDHSK4VMF","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKXUNVTF","created_at":"2026-05-18T12:25:47.102015+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/EKXUNVTFDHSK4VMFPUOTCDO4YN","json":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN.json","graph_json":"https://pith.science/api/pith-number/EKXUNVTFDHSK4VMFPUOTCDO4YN/graph.json","events_json":"https://pith.science/api/pith-number/EKXUNVTFDHSK4VMFPUOTCDO4YN/events.json","paper":"https://pith.science/paper/EKXUNVTF"},"agent_actions":{"view_html":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN","download_json":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN.json","view_paper":"https://pith.science/paper/EKXUNVTF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9209008&json=true","fetch_graph":"https://pith.science/api/pith-number/EKXUNVTFDHSK4VMFPUOTCDO4YN/graph.json","fetch_events":"https://pith.science/api/pith-number/EKXUNVTFDHSK4VMFPUOTCDO4YN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN/action/storage_attestation","attest_author":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN/action/author_attestation","sign_citation":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN/action/citation_signature","submit_replication":"https://pith.science/pith/EKXUNVTFDHSK4VMFPUOTCDO4YN/action/replication_record"}},"created_at":"2026-05-18T04:28:28.190324+00:00","updated_at":"2026-05-18T04:28:28.190324+00:00"}