{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:LUUBVMLPBSWD54FQPI5JA5RNDJ","short_pith_number":"pith:LUUBVMLP","schema_version":"1.0","canonical_sha256":"5d281ab16f0cac3ef0b07a3a90762d1a59262e8d75d2e003eef5af8f29ff054b","source":{"kind":"arxiv","id":"hep-lat/0609065","version":1},"attestation_state":"computed","paper":{"title":"m_b and f_Bs from a combination of HQET and QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Damiano Guazzini, Nazario Tantalo, Rainer Sommer","submitted_at":"2006-09-28T14:02:52Z","abstract_excerpt":"We compute the mass of the b-quark and the B_s meson decay constant in quenched lattice QCD using a combination of HQET and the standard relativistic QCD Lagrangian. We start from a small volume, where one can directly deal with the b-quark, and compute the evolution to a big volume, where the finite size effects are negligible through step scaling functions which give the change of the observables when L is changed to 2L. In all steps we extrapolate to the continuum limit, separately in HQET and in QCD for masses below m_b. The point m_b is then reached by an interpolation of the continuum re"},"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/0609065","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2006-09-28T14:02:52Z","cross_cats_sorted":[],"title_canon_sha256":"9f82ed6e40d29e4e1b5ce03962157bdd530ef65beb83f82796bece4a759c785f","abstract_canon_sha256":"0326361cbc7b4b848d6baf0cc3f6337cc4847b1e853dc845ba44943349cc0d83"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:46.546608Z","signature_b64":"9PjXKsBPEFEFnsgY5050RBiEKugnYHgX8zlGz04D5Y6e44wu4bPkl4zoLP4lFRIPOVINgoOenM/1V3MU6MJgAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d281ab16f0cac3ef0b07a3a90762d1a59262e8d75d2e003eef5af8f29ff054b","last_reissued_at":"2026-05-18T04:30:46.546189Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:46.546189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"m_b and f_Bs from a combination of HQET and QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Damiano Guazzini, Nazario Tantalo, Rainer Sommer","submitted_at":"2006-09-28T14:02:52Z","abstract_excerpt":"We compute the mass of the b-quark and the B_s meson decay constant in quenched lattice QCD using a combination of HQET and the standard relativistic QCD Lagrangian. We start from a small volume, where one can directly deal with the b-quark, and compute the evolution to a big volume, where the finite size effects are negligible through step scaling functions which give the change of the observables when L is changed to 2L. In all steps we extrapolate to the continuum limit, separately in HQET and in QCD for masses below m_b. The point m_b is then reached by an interpolation of the continuum re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0609065","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/0609065","created_at":"2026-05-18T04:30:46.546249+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0609065v1","created_at":"2026-05-18T04:30:46.546249+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0609065","created_at":"2026-05-18T04:30:46.546249+00:00"},{"alias_kind":"pith_short_12","alias_value":"LUUBVMLPBSWD","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"LUUBVMLPBSWD54FQ","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"LUUBVMLP","created_at":"2026-05-18T12:25:54.717736+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/LUUBVMLPBSWD54FQPI5JA5RNDJ","json":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ.json","graph_json":"https://pith.science/api/pith-number/LUUBVMLPBSWD54FQPI5JA5RNDJ/graph.json","events_json":"https://pith.science/api/pith-number/LUUBVMLPBSWD54FQPI5JA5RNDJ/events.json","paper":"https://pith.science/paper/LUUBVMLP"},"agent_actions":{"view_html":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ","download_json":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ.json","view_paper":"https://pith.science/paper/LUUBVMLP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0609065&json=true","fetch_graph":"https://pith.science/api/pith-number/LUUBVMLPBSWD54FQPI5JA5RNDJ/graph.json","fetch_events":"https://pith.science/api/pith-number/LUUBVMLPBSWD54FQPI5JA5RNDJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ/action/storage_attestation","attest_author":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ/action/author_attestation","sign_citation":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ/action/citation_signature","submit_replication":"https://pith.science/pith/LUUBVMLPBSWD54FQPI5JA5RNDJ/action/replication_record"}},"created_at":"2026-05-18T04:30:46.546249+00:00","updated_at":"2026-05-18T04:30:46.546249+00:00"}