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The advantages are that large CP asymmetries are expected in these processes and only singly Cabibbo-suppressed $D$ decay modes are involved. Measurements of the branching fractions of the neutral $B_d$ decays into $DK^{*}_{0(2)}(1430)$ and the time-dependent CP asymmetries in $B_s\\to (D^0, \\bar D^0) M$ ($M=f_0(980),f_0(1370), f_2'(1525), f_1(1285), f_1("},"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":"1110.5194","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-10-24T10:56:31Z","cross_cats_sorted":[],"title_canon_sha256":"27013cecbb91264d53e794f51358a6c1a5d91a029b2f55f0ef4a7eca3626459d","abstract_canon_sha256":"d6e8139328e960abbf90d8e870b25188226d5eb9a7e2aca916c746a405f94637"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:58:51.162136Z","signature_b64":"MVNOMXDileN3SAsMcC23neis95j58ncCdf2uZEqDD81nrNvUC+T3tFsty4QUvNyYKkUO1gUIppcgAV9SpOOACg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a4651a01905c21b6287bf68666891957c9ca1c4198bb8e17f7c27a31214ad18e","last_reissued_at":"2026-05-18T03:58:51.161578Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:58:51.161578Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Determining CP violation angle $\\gamma$ with B decays into a scalar/tensor meson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Wei Wang","submitted_at":"2011-10-24T10:56:31Z","abstract_excerpt":"We propose a new way for determining the CP violation angle $\\gamma$ without any hadronic uncertainty. 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Measurements of the branching fractions of the neutral $B_d$ decays into $DK^{*}_{0(2)}(1430)$ and the time-dependent CP asymmetries in $B_s\\to (D^0, \\bar D^0) M$ ($M=f_0(980),f_0(1370), f_2'(1525), f_1(1285), f_1("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.5194","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":"1110.5194","created_at":"2026-05-18T03:58:51.161670+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.5194v2","created_at":"2026-05-18T03:58:51.161670+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.5194","created_at":"2026-05-18T03:58:51.161670+00:00"},{"alias_kind":"pith_short_12","alias_value":"URSRUAMQLQQ3","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"URSRUAMQLQQ3MKD3","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"URSRUAMQ","created_at":"2026-05-18T12:26:42.757692+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.22824","citing_title":"Rotational Spectroscopy as a Tool to Study Vibration-Rotation Interaction: Investigations of $^{13}$CH$_3$CN and CH$_3$$^{13}$CN up to $v_8 = 2$ and a Search for $v_8 = 2$ Transitions toward Sagittari","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7","json":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7.json","graph_json":"https://pith.science/api/pith-number/URSRUAMQLQQ3MKD362DGNCIZK7/graph.json","events_json":"https://pith.science/api/pith-number/URSRUAMQLQQ3MKD362DGNCIZK7/events.json","paper":"https://pith.science/paper/URSRUAMQ"},"agent_actions":{"view_html":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7","download_json":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7.json","view_paper":"https://pith.science/paper/URSRUAMQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.5194&json=true","fetch_graph":"https://pith.science/api/pith-number/URSRUAMQLQQ3MKD362DGNCIZK7/graph.json","fetch_events":"https://pith.science/api/pith-number/URSRUAMQLQQ3MKD362DGNCIZK7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7/action/storage_attestation","attest_author":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7/action/author_attestation","sign_citation":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7/action/citation_signature","submit_replication":"https://pith.science/pith/URSRUAMQLQQ3MKD362DGNCIZK7/action/replication_record"}},"created_at":"2026-05-18T03:58:51.161670+00:00","updated_at":"2026-05-18T03:58:51.161670+00:00"}