{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:NZC5HMN7JB3FFTTUG7IF5WPBEQ","short_pith_number":"pith:NZC5HMN7","schema_version":"1.0","canonical_sha256":"6e45d3b1bf487652ce7437d05ed9e1241edaa9d6f1ab7956aa05f6e835e400cf","source":{"kind":"arxiv","id":"2105.11433","version":2},"attestation_state":"computed","paper":{"title":"$B_s \\rightarrow D_s^*$ Form Factors for the full $q^2$ range from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Christine T. H. Davies, Judd Harrison","submitted_at":"2021-05-24T17:41:44Z","abstract_excerpt":"We compute the Standard Model semileptonic vector and axial-vector form factors for $B_s\\to D_s^*$ decay across the full $q^2$ range using lattice QCD. We use the Highly Improved Staggered Quark (HISQ) action for all valence quarks, enabling us to normalise weak currents nonperturbatively. We use gluon field configurations including $u$, $d$, $s$ and $c$ HISQ sea quarks and multiple HISQ heavy quarks with masses from the $c$ mass up to that of the $b$ on our finest lattices. We determine the physical form factors, with which we construct the differential and total rates for $\\Gamma(B_s^0\\to D_"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2105.11433","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2021-05-24T17:41:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fad120bd484006d39e36bbc49f3549339c2ca2c8213a7d1df9e7c1c651a53493","abstract_canon_sha256":"cb94d05cc323b79acfdf0f77cf2e40ecd703fe07e5464519a1144d2071c219bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:29:24.760755Z","signature_b64":"E5FPL1bGkoBWjpGbP9OZtB/+pE5cOXP+dfWG6jTk2ff+lu31KdnbdWBWhqzIX2yrC1DG/ZeOtU98MOwpZoL3Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6e45d3b1bf487652ce7437d05ed9e1241edaa9d6f1ab7956aa05f6e835e400cf","last_reissued_at":"2026-07-05T04:29:24.760348Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:29:24.760348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B_s \\rightarrow D_s^*$ Form Factors for the full $q^2$ range from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Christine T. H. Davies, Judd Harrison","submitted_at":"2021-05-24T17:41:44Z","abstract_excerpt":"We compute the Standard Model semileptonic vector and axial-vector form factors for $B_s\\to D_s^*$ decay across the full $q^2$ range using lattice QCD. We use the Highly Improved Staggered Quark (HISQ) action for all valence quarks, enabling us to normalise weak currents nonperturbatively. We use gluon field configurations including $u$, $d$, $s$ and $c$ HISQ sea quarks and multiple HISQ heavy quarks with masses from the $c$ mass up to that of the $b$ on our finest lattices. We determine the physical form factors, with which we construct the differential and total rates for $\\Gamma(B_s^0\\to D_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.11433","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/2105.11433/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":"2105.11433","created_at":"2026-07-05T04:29:24.760407+00:00"},{"alias_kind":"arxiv_version","alias_value":"2105.11433v2","created_at":"2026-07-05T04:29:24.760407+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.11433","created_at":"2026-07-05T04:29:24.760407+00:00"},{"alias_kind":"pith_short_12","alias_value":"NZC5HMN7JB3F","created_at":"2026-07-05T04:29:24.760407+00:00"},{"alias_kind":"pith_short_16","alias_value":"NZC5HMN7JB3FFTTU","created_at":"2026-07-05T04:29:24.760407+00:00"},{"alias_kind":"pith_short_8","alias_value":"NZC5HMN7","created_at":"2026-07-05T04:29:24.760407+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/NZC5HMN7JB3FFTTUG7IF5WPBEQ","json":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ.json","graph_json":"https://pith.science/api/pith-number/NZC5HMN7JB3FFTTUG7IF5WPBEQ/graph.json","events_json":"https://pith.science/api/pith-number/NZC5HMN7JB3FFTTUG7IF5WPBEQ/events.json","paper":"https://pith.science/paper/NZC5HMN7"},"agent_actions":{"view_html":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ","download_json":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ.json","view_paper":"https://pith.science/paper/NZC5HMN7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2105.11433&json=true","fetch_graph":"https://pith.science/api/pith-number/NZC5HMN7JB3FFTTUG7IF5WPBEQ/graph.json","fetch_events":"https://pith.science/api/pith-number/NZC5HMN7JB3FFTTUG7IF5WPBEQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ/action/storage_attestation","attest_author":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ/action/author_attestation","sign_citation":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ/action/citation_signature","submit_replication":"https://pith.science/pith/NZC5HMN7JB3FFTTUG7IF5WPBEQ/action/replication_record"}},"created_at":"2026-07-05T04:29:24.760407+00:00","updated_at":"2026-07-05T04:29:24.760407+00:00"}