{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:OGCABSDXHNF3JGHV6KRCW2BJJ3","short_pith_number":"pith:OGCABSDX","schema_version":"1.0","canonical_sha256":"718400c8773b4bb498f5f2a22b68294ecac4c9faeb4a11764f696559b809a002","source":{"kind":"arxiv","id":"hep-ph/0608144","version":1},"attestation_state":"computed","paper":{"title":"New physics upper bound on the branching ratio of B_s--> l+ l- and B_s--> l+ l- gamma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ashutosh Kumar Alok, S. Uma Sankar","submitted_at":"2006-08-12T21:00:53Z","abstract_excerpt":"We consider the most general new physics effective Lagrangian for b--> s l+ l-. We derive the upper limit on the branching ratio for the processes B_s--> l^+ l- where l=e, mu, subject to the current experimental bounds on related processes, B--> (K,K*) l+ l-. If the new physics interactions are of vector/axial-vector form, the present measured rates for B--> (K,K*) l+ l- constrain B_s--> l+ l to be of the same order of magnitude as their respective Standard Model (SM) predictions. On the other hand, if the new physics interactions are of scalar/pseudoscalar form, B--> (K,K*) l+ l- rates do not"},"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/0608144","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-08-12T21:00:53Z","cross_cats_sorted":[],"title_canon_sha256":"e0f858914ad822a9fe485c78efe1b441d0b2bfb6088c436bd411403d1b7a9187","abstract_canon_sha256":"55b2a8f369d6fac91089135b610e4ab0c9f82cbef731b0392ead4bab78f675c1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:26.390603Z","signature_b64":"Rt9QLMvZYR/MhPICqLZKzhTLSvOpMlTYAGI1Rr+VKq+S6d97WoR3lIM9Xtp62VAIIhYH1W3ipWVhQAGXWCipCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"718400c8773b4bb498f5f2a22b68294ecac4c9faeb4a11764f696559b809a002","last_reissued_at":"2026-07-04T15:19:26.390223Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:26.390223Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New physics upper bound on the branching ratio of B_s--> l+ l- and B_s--> l+ l- gamma","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ashutosh Kumar Alok, S. Uma Sankar","submitted_at":"2006-08-12T21:00:53Z","abstract_excerpt":"We consider the most general new physics effective Lagrangian for b--> s l+ l-. We derive the upper limit on the branching ratio for the processes B_s--> l^+ l- where l=e, mu, subject to the current experimental bounds on related processes, B--> (K,K*) l+ l-. If the new physics interactions are of vector/axial-vector form, the present measured rates for B--> (K,K*) l+ l- constrain B_s--> l+ l to be of the same order of magnitude as their respective Standard Model (SM) predictions. On the other hand, if the new physics interactions are of scalar/pseudoscalar form, B--> (K,K*) l+ l- rates do not"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0608144","kind":"arxiv","version":1},"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/0608144/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/0608144","created_at":"2026-07-04T15:19:26.390282+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0608144v1","created_at":"2026-07-04T15:19:26.390282+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0608144","created_at":"2026-07-04T15:19:26.390282+00:00"},{"alias_kind":"pith_short_12","alias_value":"OGCABSDXHNF3","created_at":"2026-07-04T15:19:26.390282+00:00"},{"alias_kind":"pith_short_16","alias_value":"OGCABSDXHNF3JGHV","created_at":"2026-07-04T15:19:26.390282+00:00"},{"alias_kind":"pith_short_8","alias_value":"OGCABSDX","created_at":"2026-07-04T15:19:26.390282+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/OGCABSDXHNF3JGHV6KRCW2BJJ3","json":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3.json","graph_json":"https://pith.science/api/pith-number/OGCABSDXHNF3JGHV6KRCW2BJJ3/graph.json","events_json":"https://pith.science/api/pith-number/OGCABSDXHNF3JGHV6KRCW2BJJ3/events.json","paper":"https://pith.science/paper/OGCABSDX"},"agent_actions":{"view_html":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3","download_json":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3.json","view_paper":"https://pith.science/paper/OGCABSDX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0608144&json=true","fetch_graph":"https://pith.science/api/pith-number/OGCABSDXHNF3JGHV6KRCW2BJJ3/graph.json","fetch_events":"https://pith.science/api/pith-number/OGCABSDXHNF3JGHV6KRCW2BJJ3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3/action/storage_attestation","attest_author":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3/action/author_attestation","sign_citation":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3/action/citation_signature","submit_replication":"https://pith.science/pith/OGCABSDXHNF3JGHV6KRCW2BJJ3/action/replication_record"}},"created_at":"2026-07-04T15:19:26.390282+00:00","updated_at":"2026-07-04T15:19:26.390282+00:00"}