{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:3EDYZDU3CR4K4CYO3OTBY5XRZ2","short_pith_number":"pith:3EDYZDU3","schema_version":"1.0","canonical_sha256":"d9078c8e9b1478ae0b0edba61c76f1cea0b440c2248c3372fc3bf6197f2ad850","source":{"kind":"arxiv","id":"0903.0601","version":3},"attestation_state":"computed","paper":{"title":"Absolute Branching Fraction Measurements for Exclusive $D_s$ Semileptonic Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, The CLEO Collaboration: J. Yelton","submitted_at":"2009-03-03T19:28:33Z","abstract_excerpt":"We measure the absolute branching fractions of $\\Ds$ semileptonic decays where the hadron in the final state is one of $\\phi$, $\\eta$, $\\etap$, $\\Ks$, $\\Kstar$, and $f_0$, using $2.8 \\times 10^5$ $\\epm \\to \\Ds\\Dsstar$ decays collected in the CLEO-c detector at a center-of-mass energy close to 4170 MeV. We obtain ${\\cal B}(\\Dsp\\to \\phi e^+ \\nu_e) =(2.29\\pm 0.37 \\pm 0.11)$%, ${\\cal B}(\\Dsp\\to \\eta e^+ \\nu_e) =(2.48 \\pm 0.29 \\pm 0.13)$%, ${\\cal B}(\\Dsp\\to \\etap e^+ \\nu_e) =(0.91 \\pm 0.33 \\pm 0.05)$%, where the first uncertainties are statistical and the second are systematic. We also obtain ${\\ca"},"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":"0903.0601","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2009-03-03T19:28:33Z","cross_cats_sorted":[],"title_canon_sha256":"1c98fffccb85b5f078409f39a7a7a1765c605189e9698239bc6e6318e74604e0","abstract_canon_sha256":"81b7cf9db5347e65f611db32b97fdc76391551ebe527b5d53418b9a2952d6b8b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:25:49.354454Z","signature_b64":"430ngZraDxvNM51ycaFuS5asiY5TalGT+GkkNx4LJkFGk+V6v3ShqWlDA6jQfR2o9vHbgU5j5TVceSzX0ESIBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9078c8e9b1478ae0b0edba61c76f1cea0b440c2248c3372fc3bf6197f2ad850","last_reissued_at":"2026-07-04T17:25:49.354076Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:25:49.354076Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Absolute Branching Fraction Measurements for Exclusive $D_s$ Semileptonic Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, The CLEO Collaboration: J. Yelton","submitted_at":"2009-03-03T19:28:33Z","abstract_excerpt":"We measure the absolute branching fractions of $\\Ds$ semileptonic decays where the hadron in the final state is one of $\\phi$, $\\eta$, $\\etap$, $\\Ks$, $\\Kstar$, and $f_0$, using $2.8 \\times 10^5$ $\\epm \\to \\Ds\\Dsstar$ decays collected in the CLEO-c detector at a center-of-mass energy close to 4170 MeV. We obtain ${\\cal B}(\\Dsp\\to \\phi e^+ \\nu_e) =(2.29\\pm 0.37 \\pm 0.11)$%, ${\\cal B}(\\Dsp\\to \\eta e^+ \\nu_e) =(2.48 \\pm 0.29 \\pm 0.13)$%, ${\\cal B}(\\Dsp\\to \\etap e^+ \\nu_e) =(0.91 \\pm 0.33 \\pm 0.05)$%, where the first uncertainties are statistical and the second are systematic. We also obtain ${\\ca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.0601","kind":"arxiv","version":3},"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/0903.0601/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":"0903.0601","created_at":"2026-07-04T17:25:49.354137+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.0601v3","created_at":"2026-07-04T17:25:49.354137+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.0601","created_at":"2026-07-04T17:25:49.354137+00:00"},{"alias_kind":"pith_short_12","alias_value":"3EDYZDU3CR4K","created_at":"2026-07-04T17:25:49.354137+00:00"},{"alias_kind":"pith_short_16","alias_value":"3EDYZDU3CR4K4CYO","created_at":"2026-07-04T17:25:49.354137+00:00"},{"alias_kind":"pith_short_8","alias_value":"3EDYZDU3","created_at":"2026-07-04T17:25:49.354137+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.18075","citing_title":"Compact $cs\\bar{s}\\bar{s}$ Tetraquarks in the Charm--Strange Sector: Mass Spectra, Rearrangement Decays and Regge Trajectories with $D_s$ Threshold Inputs","ref_index":82,"is_internal_anchor":true},{"citing_arxiv_id":"2604.20644","citing_title":"Review of experimental studies of charmed meson decays at BESIII","ref_index":192,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2","json":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2.json","graph_json":"https://pith.science/api/pith-number/3EDYZDU3CR4K4CYO3OTBY5XRZ2/graph.json","events_json":"https://pith.science/api/pith-number/3EDYZDU3CR4K4CYO3OTBY5XRZ2/events.json","paper":"https://pith.science/paper/3EDYZDU3"},"agent_actions":{"view_html":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2","download_json":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2.json","view_paper":"https://pith.science/paper/3EDYZDU3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.0601&json=true","fetch_graph":"https://pith.science/api/pith-number/3EDYZDU3CR4K4CYO3OTBY5XRZ2/graph.json","fetch_events":"https://pith.science/api/pith-number/3EDYZDU3CR4K4CYO3OTBY5XRZ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2/action/storage_attestation","attest_author":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2/action/author_attestation","sign_citation":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2/action/citation_signature","submit_replication":"https://pith.science/pith/3EDYZDU3CR4K4CYO3OTBY5XRZ2/action/replication_record"}},"created_at":"2026-07-04T17:25:49.354137+00:00","updated_at":"2026-07-04T17:25:49.354137+00:00"}