{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:IHR6IM72SFW275UK2DNH46SF5Q","short_pith_number":"pith:IHR6IM72","schema_version":"1.0","canonical_sha256":"41e3e433fa916daff68ad0da7e7a45ec2453499137af4d9061c4589b2f663e8b","source":{"kind":"arxiv","id":"1701.03923","version":2},"attestation_state":"computed","paper":{"title":"Form factors in the $\\mathrm{B}_\\mathrm{s} \\rightarrow \\mathrm{K} \\ell \\nu$ decays using HQET and the lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Debasish Banerjee","submitted_at":"2017-01-14T13:57:40Z","abstract_excerpt":"We report on a recent computation of the form factors in semi-leptonic decays of the $\\mathrm{B}_\\mathrm{s}$ using Heavy Quark Effective Theory (HQET) formalism applied on the lattice. The connection of the form factors with the 2-point and 3-point correlators on the lattice is explained, and the subsequent non-perturbative renormalization of HQET and it's matching to $N_f=2$ QCD is outlined. The results of the (static) leading-order calculation in the continuum limit is presented."},"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":"1701.03923","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-01-14T13:57:40Z","cross_cats_sorted":[],"title_canon_sha256":"4270192796d67d6fe221d1d54b126c84b6723ef3ef5bb58c6c33d4b451bbaaf1","abstract_canon_sha256":"394c5c83adb65e783164fb0b39ce4fd154d018c50a6736192bc65937a5481269"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:43.805276Z","signature_b64":"I8UfLakmEVgjTS5BIZTMY26HnHjUZuVXnKtAMWFJZZibfcJejcgfflJc1kNVyLUoxt3Y/eRN+72EXmBAhDo4Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"41e3e433fa916daff68ad0da7e7a45ec2453499137af4d9061c4589b2f663e8b","last_reissued_at":"2026-05-18T00:52:43.804804Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:43.804804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Form factors in the $\\mathrm{B}_\\mathrm{s} \\rightarrow \\mathrm{K} \\ell \\nu$ decays using HQET and the lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Debasish Banerjee","submitted_at":"2017-01-14T13:57:40Z","abstract_excerpt":"We report on a recent computation of the form factors in semi-leptonic decays of the $\\mathrm{B}_\\mathrm{s}$ using Heavy Quark Effective Theory (HQET) formalism applied on the lattice. The connection of the form factors with the 2-point and 3-point correlators on the lattice is explained, and the subsequent non-perturbative renormalization of HQET and it's matching to $N_f=2$ QCD is outlined. The results of the (static) leading-order calculation in the continuum limit is presented."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.03923","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":""},"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":"1701.03923","created_at":"2026-05-18T00:52:43.804893+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.03923v2","created_at":"2026-05-18T00:52:43.804893+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.03923","created_at":"2026-05-18T00:52:43.804893+00:00"},{"alias_kind":"pith_short_12","alias_value":"IHR6IM72SFW2","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"IHR6IM72SFW275UK","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"IHR6IM72","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.05104","citing_title":"Weak decays of $B_s$ meson in self-consistent covariant light-front approach","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q","json":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q.json","graph_json":"https://pith.science/api/pith-number/IHR6IM72SFW275UK2DNH46SF5Q/graph.json","events_json":"https://pith.science/api/pith-number/IHR6IM72SFW275UK2DNH46SF5Q/events.json","paper":"https://pith.science/paper/IHR6IM72"},"agent_actions":{"view_html":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q","download_json":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q.json","view_paper":"https://pith.science/paper/IHR6IM72","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.03923&json=true","fetch_graph":"https://pith.science/api/pith-number/IHR6IM72SFW275UK2DNH46SF5Q/graph.json","fetch_events":"https://pith.science/api/pith-number/IHR6IM72SFW275UK2DNH46SF5Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q/action/storage_attestation","attest_author":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q/action/author_attestation","sign_citation":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q/action/citation_signature","submit_replication":"https://pith.science/pith/IHR6IM72SFW275UK2DNH46SF5Q/action/replication_record"}},"created_at":"2026-05-18T00:52:43.804893+00:00","updated_at":"2026-05-18T00:52:43.804893+00:00"}