{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:4HQLGJHBZYCCPB3RMQKYRNBZOT","short_pith_number":"pith:4HQLGJHB","schema_version":"1.0","canonical_sha256":"e1e0b324e1ce04278771641588b43974cdd0e788b6a2c03ff5ab9b5f29e1b849","source":{"kind":"arxiv","id":"1110.2099","version":1},"attestation_state":"computed","paper":{"title":"Updated Measurement of ${\\cal B}(B_s \\to D_s^{(*)+}D_s^{(*)-})$ and Determination of $\\Delta \\Gamma_{s}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Sevda Esen","submitted_at":"2011-10-10T16:39:18Z","abstract_excerpt":"Using fully reconstructed $B_{s}$ mesons, we measure exclusive branching fractions for the decays $B_s \\to D_s^{(*)+}D_s^{(*)-}$. The results are ${\\cal B}(B^0_s\\ra D^+_s D^-_s)=(0.58\\,^{+0.11}_{-0.09}\\,\\pm 0.13)%$, ${\\cal B}(B^0_s\\ra D^{*\\pm}_s D^{\\mp}_s)=(1.8\\, \\pm 0.2\\,\\pm 0.4)%$, and ${\\cal B}(B^0_s\\ra D^{*+}_s D^{*-}_s)=(2.0\\,\\pm 0.3\\,\\pm 0.5)%$; the sum is ${\\cal B}(B^0_s\\ra D^{(*)+}_s D^{(*)-}_s)=(4.3\\,\\pm 0.4\\,\\pm 1.0)%$. Assuming these decay modes saturate decays to CP-even final states, the branching fraction determines the relative width difference between the $B_s$ CP-odd and CP-ev"},"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":"1110.2099","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-10-10T16:39:18Z","cross_cats_sorted":[],"title_canon_sha256":"469e82875c5275d83e04718aeff48ef93fbd8de2811c4c5ed16edcd481edfcab","abstract_canon_sha256":"f5767081bcf1155d791f205851a24a0b79cde6bccf6d4e901d176817e881d76b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:11:18.965685Z","signature_b64":"6zBYIZ9YQesO39GTwvhvNc0EAtVHAfLSvq78eyvHhhqckJBa5QoKON9aFAU6svPgaseZJcDUpg/cTpipLOaSDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1e0b324e1ce04278771641588b43974cdd0e788b6a2c03ff5ab9b5f29e1b849","last_reissued_at":"2026-05-18T04:11:18.964999Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:11:18.964999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Updated Measurement of ${\\cal B}(B_s \\to D_s^{(*)+}D_s^{(*)-})$ and Determination of $\\Delta \\Gamma_{s}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Sevda Esen","submitted_at":"2011-10-10T16:39:18Z","abstract_excerpt":"Using fully reconstructed $B_{s}$ mesons, we measure exclusive branching fractions for the decays $B_s \\to D_s^{(*)+}D_s^{(*)-}$. The results are ${\\cal B}(B^0_s\\ra D^+_s D^-_s)=(0.58\\,^{+0.11}_{-0.09}\\,\\pm 0.13)%$, ${\\cal B}(B^0_s\\ra D^{*\\pm}_s D^{\\mp}_s)=(1.8\\, \\pm 0.2\\,\\pm 0.4)%$, and ${\\cal B}(B^0_s\\ra D^{*+}_s D^{*-}_s)=(2.0\\,\\pm 0.3\\,\\pm 0.5)%$; the sum is ${\\cal B}(B^0_s\\ra D^{(*)+}_s D^{(*)-}_s)=(4.3\\,\\pm 0.4\\,\\pm 1.0)%$. Assuming these decay modes saturate decays to CP-even final states, the branching fraction determines the relative width difference between the $B_s$ CP-odd and CP-ev"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.2099","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":""},"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":"1110.2099","created_at":"2026-05-18T04:11:18.965099+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.2099v1","created_at":"2026-05-18T04:11:18.965099+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.2099","created_at":"2026-05-18T04:11:18.965099+00:00"},{"alias_kind":"pith_short_12","alias_value":"4HQLGJHBZYCC","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"4HQLGJHBZYCCPB3R","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"4HQLGJHB","created_at":"2026-05-18T12:26:20.644004+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/4HQLGJHBZYCCPB3RMQKYRNBZOT","json":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT.json","graph_json":"https://pith.science/api/pith-number/4HQLGJHBZYCCPB3RMQKYRNBZOT/graph.json","events_json":"https://pith.science/api/pith-number/4HQLGJHBZYCCPB3RMQKYRNBZOT/events.json","paper":"https://pith.science/paper/4HQLGJHB"},"agent_actions":{"view_html":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT","download_json":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT.json","view_paper":"https://pith.science/paper/4HQLGJHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.2099&json=true","fetch_graph":"https://pith.science/api/pith-number/4HQLGJHBZYCCPB3RMQKYRNBZOT/graph.json","fetch_events":"https://pith.science/api/pith-number/4HQLGJHBZYCCPB3RMQKYRNBZOT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT/action/storage_attestation","attest_author":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT/action/author_attestation","sign_citation":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT/action/citation_signature","submit_replication":"https://pith.science/pith/4HQLGJHBZYCCPB3RMQKYRNBZOT/action/replication_record"}},"created_at":"2026-05-18T04:11:18.965099+00:00","updated_at":"2026-05-18T04:11:18.965099+00:00"}