{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:FGGOEHF3GC7WLEFNJM7NJQBP7N","short_pith_number":"pith:FGGOEHF3","schema_version":"1.0","canonical_sha256":"298ce21cbb30bf6590ad4b3ed4c02ffb6efe7159a1bff253114ff68bc8992ca6","source":{"kind":"arxiv","id":"1011.5979","version":4},"attestation_state":"computed","paper":{"title":"Like-sign dimuon charge asymmetry in Randall-Sundurm model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alakabha Datta, Murugeswaran Duraisamy, Shaaban Khalil","submitted_at":"2010-11-27T16:10:04Z","abstract_excerpt":"We confirm that in order to account for the recent D\\O\\ result of large like-sign dimuon charge asymmetry, a considerable large new physics effect in $\\Gamma_{12}^s$ is required in addition to a large CP violating phase in $B_s -\\bar{B}_s$ mixing. In the Randall-Sundrum model of warped geometry, where the fermion fields reside in the bulk, new sources of flavor and CP violation are obtained. We analyze the like-sign dimuon asymmetry in this class of model, as an example of the desired new physics. We show that the wrong charge asymmetry, $a_{sl}^s$, which is related to the dimuon asymmetry, is"},"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":"1011.5979","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-27T16:10:04Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"1c628d54beee67d4ff9f83df1608c7d37c199b97e9be68d0e4430d0a8d348843","abstract_canon_sha256":"22f76cf9c3d13d1d27e20561e4d742c4d94696b1e4af6e57ce02e77f7fd61e8f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:23:17.381779Z","signature_b64":"UoZzMxz31WCX8HPRlKvUot9GGHY7+wwH27G/lu3j52Zv9ukQDDvPUPIxSMUNpVxB8TqjVmBiE8rVJq2AbeApCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"298ce21cbb30bf6590ad4b3ed4c02ffb6efe7159a1bff253114ff68bc8992ca6","last_reissued_at":"2026-05-18T02:23:17.381185Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:23:17.381185Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Like-sign dimuon charge asymmetry in Randall-Sundurm model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alakabha Datta, Murugeswaran Duraisamy, Shaaban Khalil","submitted_at":"2010-11-27T16:10:04Z","abstract_excerpt":"We confirm that in order to account for the recent D\\O\\ result of large like-sign dimuon charge asymmetry, a considerable large new physics effect in $\\Gamma_{12}^s$ is required in addition to a large CP violating phase in $B_s -\\bar{B}_s$ mixing. In the Randall-Sundrum model of warped geometry, where the fermion fields reside in the bulk, new sources of flavor and CP violation are obtained. We analyze the like-sign dimuon asymmetry in this class of model, as an example of the desired new physics. We show that the wrong charge asymmetry, $a_{sl}^s$, which is related to the dimuon asymmetry, is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.5979","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":"1011.5979","created_at":"2026-05-18T02:23:17.381259+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.5979v4","created_at":"2026-05-18T02:23:17.381259+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.5979","created_at":"2026-05-18T02:23:17.381259+00:00"},{"alias_kind":"pith_short_12","alias_value":"FGGOEHF3GC7W","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_16","alias_value":"FGGOEHF3GC7WLEFN","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_8","alias_value":"FGGOEHF3","created_at":"2026-05-18T12:26:07.630475+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/FGGOEHF3GC7WLEFNJM7NJQBP7N","json":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N.json","graph_json":"https://pith.science/api/pith-number/FGGOEHF3GC7WLEFNJM7NJQBP7N/graph.json","events_json":"https://pith.science/api/pith-number/FGGOEHF3GC7WLEFNJM7NJQBP7N/events.json","paper":"https://pith.science/paper/FGGOEHF3"},"agent_actions":{"view_html":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N","download_json":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N.json","view_paper":"https://pith.science/paper/FGGOEHF3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.5979&json=true","fetch_graph":"https://pith.science/api/pith-number/FGGOEHF3GC7WLEFNJM7NJQBP7N/graph.json","fetch_events":"https://pith.science/api/pith-number/FGGOEHF3GC7WLEFNJM7NJQBP7N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N/action/storage_attestation","attest_author":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N/action/author_attestation","sign_citation":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N/action/citation_signature","submit_replication":"https://pith.science/pith/FGGOEHF3GC7WLEFNJM7NJQBP7N/action/replication_record"}},"created_at":"2026-05-18T02:23:17.381259+00:00","updated_at":"2026-05-18T02:23:17.381259+00:00"}