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Light quark propagators were calculated using the $O(a)$-improved Sheikholeslami-Wohlert action. We find $\\Bbstat(m_b) = 0.69\\er{3}{4} {\\rm(stat)}\\er{2}{1} {\\rm(syst)}$, corresponding to $\\Bbstat = 1.02\\er{5}{6}\\er{3}{2}$, and $\\fbstat = 266\\err{18}{20}\\err{28}{27} \\mev$, $f_{B_s}^2 B_{B_s}/f_B^2 B_B = 1.34\\er{9}{8}\\er{5}{"},"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/9508030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1995-08-29T17:40:26Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3401f0a66f8f1573efc4731d2fd2e49694708b33d4fbd3ca48065e2d8fc9c491","abstract_canon_sha256":"9b48ae7565f2bc25608366d55baf6dc1e8394f71810b9b0ccea4ac148e56ea25"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:29:30.473662Z","signature_b64":"hA1g/ZFOnST5fs7QgiwsFb2bwTZV4cAP4uKTYg6AozAJQf8+dYQEsRyd0IO0wSzwKwj0jzLyYQatoua19NrODA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4ee9e37cb1372d88fa6fbfb177f361a883ce678ef87563ff42175cd1ac3d693","last_reissued_at":"2026-07-04T15:29:30.473258Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:29:30.473258Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Quark Spectroscopy and Matrix Elements: A Lattice Study using the Static Approximation","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. 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We find $\\Bbstat(m_b) = 0.69\\er{3}{4} {\\rm(stat)}\\er{2}{1} {\\rm(syst)}$, corresponding to $\\Bbstat = 1.02\\er{5}{6}\\er{3}{2}$, and $\\fbstat = 266\\err{18}{20}\\err{28}{27} \\mev$, $f_{B_s}^2 B_{B_s}/f_B^2 B_B = 1.34\\er{9}{8}\\er{5}{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9508030","kind":"arxiv","version":2},"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/9508030/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/9508030","created_at":"2026-07-04T15:29:30.473322+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9508030v2","created_at":"2026-07-04T15:29:30.473322+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9508030","created_at":"2026-07-04T15:29:30.473322+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TXJ4N6LCNZN","created_at":"2026-07-04T15:29:30.473322+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TXJ4N6LCNZNRD5G","created_at":"2026-07-04T15:29:30.473322+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TXJ4N6L","created_at":"2026-07-04T15:29:30.473322+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1909.01370","citing_title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK","json":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK.json","graph_json":"https://pith.science/api/pith-number/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/graph.json","events_json":"https://pith.science/api/pith-number/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/events.json","paper":"https://pith.science/paper/4TXJ4N6L"},"agent_actions":{"view_html":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK","download_json":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK.json","view_paper":"https://pith.science/paper/4TXJ4N6L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9508030&json=true","fetch_graph":"https://pith.science/api/pith-number/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/graph.json","fetch_events":"https://pith.science/api/pith-number/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/action/storage_attestation","attest_author":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/action/author_attestation","sign_citation":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/action/citation_signature","submit_replication":"https://pith.science/pith/4TXJ4N6LCNZNRD5G7P5RO7ZWDK/action/replication_record"}},"created_at":"2026-07-04T15:29:30.473322+00:00","updated_at":"2026-07-04T15:29:30.473322+00:00"}