{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:WA72IYHKDPS6HXVALOWDIOUMHK","short_pith_number":"pith:WA72IYHK","schema_version":"1.0","canonical_sha256":"b03fa460ea1be5e3dea05bac343a8c3a97285fd283960df59eca1d31ed8e498a","source":{"kind":"arxiv","id":"hep-ph/0703162","version":2},"attestation_state":"computed","paper":{"title":"Charmless non-leptonic B_s decays to PP, PV and VV final states in the pQCD approach","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmed Ali, Cai-Dian Lu, Gustav Kramer, Wei Wang, Ying Li, Yue-Long Shen, Yu-Ming Wang","submitted_at":"2007-03-15T11:24:22Z","abstract_excerpt":"We calculate the CP-averaged branching ratios and CP-violating asymmetries of a number of two-body charmless hadronic decays $\\bar{B_s^0} \\to PP, PV, VV$ in the perturbative QCD (pQCD) approach to leading order in $\\alpha_s$ (here $P$ and $V$ denote light pseudoscalar and vector mesons, respectively). The mixing-induced CP violation parameters are also calculated for these decays. We also predict the polarization fractions of $B_s \\to VV$ decays and find that the transverse polarizations are enhanced in some penguin dominated decays such as $\\bar{B_s^0} \\to K ^{*}\\bar{K^{*}}$, $K ^{*}\\rho$. So"},"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-ph/0703162","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-03-15T11:24:22Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bbfc9c221746f050a6eea21198034ac0f8c8463f96d83a5de76d670855b57660","abstract_canon_sha256":"68897fa88c65cb55d7005a08a1ab0b90c242576e1283a832bdcebab84751ca76"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:25:15.606659Z","signature_b64":"WcEm+Q80AVNQjqWKns6EvxDfF7mya/pBrpEWz56/vA8/vZRa0qQweoPXv6jdyiz07XY11FvIR8010H8hjipZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b03fa460ea1be5e3dea05bac343a8c3a97285fd283960df59eca1d31ed8e498a","last_reissued_at":"2026-07-04T15:25:15.606208Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:25:15.606208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charmless non-leptonic B_s decays to PP, PV and VV final states in the pQCD approach","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmed Ali, Cai-Dian Lu, Gustav Kramer, Wei Wang, Ying Li, Yue-Long Shen, Yu-Ming Wang","submitted_at":"2007-03-15T11:24:22Z","abstract_excerpt":"We calculate the CP-averaged branching ratios and CP-violating asymmetries of a number of two-body charmless hadronic decays $\\bar{B_s^0} \\to PP, PV, VV$ in the perturbative QCD (pQCD) approach to leading order in $\\alpha_s$ (here $P$ and $V$ denote light pseudoscalar and vector mesons, respectively). The mixing-induced CP violation parameters are also calculated for these decays. We also predict the polarization fractions of $B_s \\to VV$ decays and find that the transverse polarizations are enhanced in some penguin dominated decays such as $\\bar{B_s^0} \\to K ^{*}\\bar{K^{*}}$, $K ^{*}\\rho$. So"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0703162","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/hep-ph/0703162/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-ph/0703162","created_at":"2026-07-04T15:25:15.606271+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0703162v2","created_at":"2026-07-04T15:25:15.606271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0703162","created_at":"2026-07-04T15:25:15.606271+00:00"},{"alias_kind":"pith_short_12","alias_value":"WA72IYHKDPS6","created_at":"2026-07-04T15:25:15.606271+00:00"},{"alias_kind":"pith_short_16","alias_value":"WA72IYHKDPS6HXVA","created_at":"2026-07-04T15:25:15.606271+00:00"},{"alias_kind":"pith_short_8","alias_value":"WA72IYHK","created_at":"2026-07-04T15:25:15.606271+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.07776","citing_title":"B Meson Semi-Invisible Decays via Perturbative QCD","ref_index":66,"is_internal_anchor":true},{"citing_arxiv_id":"2601.01305","citing_title":"$B_c$ meson decays into $S$-wave charmonium plus light meson pairs in the perturbative QCD approach","ref_index":118,"is_internal_anchor":true},{"citing_arxiv_id":"2605.07586","citing_title":"Evidence for the decay $B^0_s\\to\\phi\\eta'$","ref_index":2,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK","json":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK.json","graph_json":"https://pith.science/api/pith-number/WA72IYHKDPS6HXVALOWDIOUMHK/graph.json","events_json":"https://pith.science/api/pith-number/WA72IYHKDPS6HXVALOWDIOUMHK/events.json","paper":"https://pith.science/paper/WA72IYHK"},"agent_actions":{"view_html":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK","download_json":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK.json","view_paper":"https://pith.science/paper/WA72IYHK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0703162&json=true","fetch_graph":"https://pith.science/api/pith-number/WA72IYHKDPS6HXVALOWDIOUMHK/graph.json","fetch_events":"https://pith.science/api/pith-number/WA72IYHKDPS6HXVALOWDIOUMHK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK/action/storage_attestation","attest_author":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK/action/author_attestation","sign_citation":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK/action/citation_signature","submit_replication":"https://pith.science/pith/WA72IYHKDPS6HXVALOWDIOUMHK/action/replication_record"}},"created_at":"2026-07-04T15:25:15.606271+00:00","updated_at":"2026-07-04T15:25:15.606271+00:00"}