{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:MGS3UCZJNFXTFE3JWJERPJS46I","short_pith_number":"pith:MGS3UCZJ","schema_version":"1.0","canonical_sha256":"61a5ba0b29696f329369b24917a65cf207538c798463f2080409c132641a3dd9","source":{"kind":"arxiv","id":"hep-lat/0608005","version":1},"attestation_state":"computed","paper":{"title":"Non-perturbatively Determined Relativistic Heavy Quark Action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Huey-Wen Lin, Norman Christ","submitted_at":"2006-08-09T01:31:41Z","abstract_excerpt":"We present a method to non-perturbatively determine the parameters of the on-shell, $O(a)$-improved relativistic heavy quark action. These three parameters, $m_0$, $\\zeta$, and $c_B=c_E$ are obtained by matching finite-volume, heavy-heavy and heavy-light meson masses to the exact relativistic spectrum through a finite-volume, step-scaling recursion procedure. We demonstrate that accuracy on the level of a few percent can be achieved by carrying out this matching on a pair of lattices with equal physical spatial volumes but quite different lattice spacings. A fine lattice with inverse lattice s"},"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/0608005","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2006-08-09T01:31:41Z","cross_cats_sorted":[],"title_canon_sha256":"499c3a33e199c28c257ab0fc7eee2a287dfebbbc45bf7276252770bdc6cfee5d","abstract_canon_sha256":"fdcd09b656a0e4297d0bb47f5df9ea827ed1ccae962ca6939fba0bb61e7b21d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:24.629256Z","signature_b64":"4SgO97Jw/vTI93Qj9c29eKNvyitScuvUoKiYd6KUiqH5I0SApqP+js8FejIg/Iltzyhut4ERDbfdudRT4byzDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61a5ba0b29696f329369b24917a65cf207538c798463f2080409c132641a3dd9","last_reissued_at":"2026-07-04T15:22:24.628860Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:24.628860Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbatively Determined Relativistic Heavy Quark Action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Huey-Wen Lin, Norman Christ","submitted_at":"2006-08-09T01:31:41Z","abstract_excerpt":"We present a method to non-perturbatively determine the parameters of the on-shell, $O(a)$-improved relativistic heavy quark action. These three parameters, $m_0$, $\\zeta$, and $c_B=c_E$ are obtained by matching finite-volume, heavy-heavy and heavy-light meson masses to the exact relativistic spectrum through a finite-volume, step-scaling recursion procedure. We demonstrate that accuracy on the level of a few percent can be achieved by carrying out this matching on a pair of lattices with equal physical spatial volumes but quite different lattice spacings. A fine lattice with inverse lattice s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0608005","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/0608005/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/0608005","created_at":"2026-07-04T15:22:24.628923+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0608005v1","created_at":"2026-07-04T15:22:24.628923+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0608005","created_at":"2026-07-04T15:22:24.628923+00:00"},{"alias_kind":"pith_short_12","alias_value":"MGS3UCZJNFXT","created_at":"2026-07-04T15:22:24.628923+00:00"},{"alias_kind":"pith_short_16","alias_value":"MGS3UCZJNFXTFE3J","created_at":"2026-07-04T15:22:24.628923+00:00"},{"alias_kind":"pith_short_8","alias_value":"MGS3UCZJ","created_at":"2026-07-04T15:22:24.628923+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.01116","citing_title":"Inclusive $\\bar B_s\\mapsto X_{\\bar sc} \\ell \\bar \\nu$ decays from lattice QCD: computational strategy and a first physical result","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I","json":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I.json","graph_json":"https://pith.science/api/pith-number/MGS3UCZJNFXTFE3JWJERPJS46I/graph.json","events_json":"https://pith.science/api/pith-number/MGS3UCZJNFXTFE3JWJERPJS46I/events.json","paper":"https://pith.science/paper/MGS3UCZJ"},"agent_actions":{"view_html":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I","download_json":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I.json","view_paper":"https://pith.science/paper/MGS3UCZJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0608005&json=true","fetch_graph":"https://pith.science/api/pith-number/MGS3UCZJNFXTFE3JWJERPJS46I/graph.json","fetch_events":"https://pith.science/api/pith-number/MGS3UCZJNFXTFE3JWJERPJS46I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I/action/storage_attestation","attest_author":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I/action/author_attestation","sign_citation":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I/action/citation_signature","submit_replication":"https://pith.science/pith/MGS3UCZJNFXTFE3JWJERPJS46I/action/replication_record"}},"created_at":"2026-07-04T15:22:24.628923+00:00","updated_at":"2026-07-04T15:22:24.628923+00:00"}