{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:PWWCWYFD2NQNTJTQY3MOAOIEWO","short_pith_number":"pith:PWWCWYFD","schema_version":"1.0","canonical_sha256":"7dac2b60a3d360d9a670c6d8e03904b3998c61ffb575222b16afc914bf66db4d","source":{"kind":"arxiv","id":"1106.3003","version":4},"attestation_state":"computed","paper":{"title":"Estimating Form Factors of $B_s\\rightarrow D_s^{(*)}$ and their Applications to Semi-leptonic and Non-leptonic Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Guo-Li Wang, Hui-feng Fu, Xiang-Jun Chen","submitted_at":"2011-06-15T15:44:34Z","abstract_excerpt":"$B_s^0\\rightarrow D_s^{-}$ and $B_s^0\\rightarrow D_s^{*-}$ weak transition form factors are estimated for the whole physical region with a method based on an instantaneous approximated Mandelstam formulation of transition matrix elements and the instantaneous Bethe-Salpeter equation. We apply the estimated form factors to branching ratios, CP asymmetries and polarization fractions of non-leptonic decays within the factorization approximation. And we study the non-factorizable effects and annihilation contributions with the perturbative QCD approach. The branching ratios of semi-leptonic $B_s^0"},"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":"1106.3003","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-06-15T15:44:34Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4863b2ad9163261e2f21116f96211b25cb2a5fe1dbe0398bb4f9ea578bd2cd7c","abstract_canon_sha256":"666a8e8e5822be0baf6e3a9cdfd1a3bc84332cd5962d72d04e4b6679e49a3b84"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:36.865303Z","signature_b64":"nCPY+vk/KrX4MxTPld39xnICqOPDAeHW0BGf1Oc3scvRrnX0JgmhQto87RE7xhchivnGYgui+wEU8Ms95V2hDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7dac2b60a3d360d9a670c6d8e03904b3998c61ffb575222b16afc914bf66db4d","last_reissued_at":"2026-05-18T02:01:36.864762Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:36.864762Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Estimating Form Factors of $B_s\\rightarrow D_s^{(*)}$ and their Applications to Semi-leptonic and Non-leptonic Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Guo-Li Wang, Hui-feng Fu, Xiang-Jun Chen","submitted_at":"2011-06-15T15:44:34Z","abstract_excerpt":"$B_s^0\\rightarrow D_s^{-}$ and $B_s^0\\rightarrow D_s^{*-}$ weak transition form factors are estimated for the whole physical region with a method based on an instantaneous approximated Mandelstam formulation of transition matrix elements and the instantaneous Bethe-Salpeter equation. We apply the estimated form factors to branching ratios, CP asymmetries and polarization fractions of non-leptonic decays within the factorization approximation. And we study the non-factorizable effects and annihilation contributions with the perturbative QCD approach. The branching ratios of semi-leptonic $B_s^0"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.3003","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1106.3003","created_at":"2026-05-18T02:01:36.864842+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.3003v4","created_at":"2026-05-18T02:01:36.864842+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.3003","created_at":"2026-05-18T02:01:36.864842+00:00"},{"alias_kind":"pith_short_12","alias_value":"PWWCWYFD2NQN","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"PWWCWYFD2NQNTJTQ","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"PWWCWYFD","created_at":"2026-05-18T12:26:39.201973+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.13456","citing_title":"$D_{(s)}(2S)$ and $D^{*}_{(s)}(2S)$ production in nonleptonic $B_{(s)}$ weak decays","ref_index":72,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO","json":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO.json","graph_json":"https://pith.science/api/pith-number/PWWCWYFD2NQNTJTQY3MOAOIEWO/graph.json","events_json":"https://pith.science/api/pith-number/PWWCWYFD2NQNTJTQY3MOAOIEWO/events.json","paper":"https://pith.science/paper/PWWCWYFD"},"agent_actions":{"view_html":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO","download_json":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO.json","view_paper":"https://pith.science/paper/PWWCWYFD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.3003&json=true","fetch_graph":"https://pith.science/api/pith-number/PWWCWYFD2NQNTJTQY3MOAOIEWO/graph.json","fetch_events":"https://pith.science/api/pith-number/PWWCWYFD2NQNTJTQY3MOAOIEWO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO/action/storage_attestation","attest_author":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO/action/author_attestation","sign_citation":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO/action/citation_signature","submit_replication":"https://pith.science/pith/PWWCWYFD2NQNTJTQY3MOAOIEWO/action/replication_record"}},"created_at":"2026-05-18T02:01:36.864842+00:00","updated_at":"2026-05-18T02:01:36.864842+00:00"}