{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:QZ5WP2LHBPBOJLOLLC7C3FLEAS","short_pith_number":"pith:QZ5WP2LH","schema_version":"1.0","canonical_sha256":"867b67e9670bc2e4adcb58be2d956404a3eb3e92d201eadec0deeeecac575f31","source":{"kind":"arxiv","id":"1011.4190","version":2},"attestation_state":"computed","paper":{"title":"Dalitz plot analysis of Ds+ --> K+ K- pi+","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"P. del Amo Sanchez et al. (The BABAR Collaboration)","submitted_at":"2010-11-18T13:50:13Z","abstract_excerpt":"We perform a Dalitz plot analysis of about 100,000 Ds+ decays to K+ K- pi+ and measure the complex amplitudes of the intermediate resonances which contribute to this decay mode. We also measure the relative branching fractions of Ds+ --> K+ K+ pi- and Ds+ --> K+ K+ K-. For this analysis we use a 384 fb-1 data sample, recorded by the BABAR detector at the PEP-II asymmetric-energy e+e- collider running at center-of-mass energies near 10.58 GeV."},"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":"1011.4190","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-11-18T13:50:13Z","cross_cats_sorted":[],"title_canon_sha256":"a335c507e5ead04c72612f23caff2cc47d490655bdb2049395f61a6f0b213e84","abstract_canon_sha256":"23e472406e3269721bd1ef05cdc07adfd37f9dc07bdfc6beeb5be073e3359898"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:27:06.368017Z","signature_b64":"eyuIVy1AsMkRiqr/M487oZGrvzR9Z92d7GIwdBEWZpvhcRcKiqeA1N5czAyat5A/vD5UjZyrbyOtIob3dXJhCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"867b67e9670bc2e4adcb58be2d956404a3eb3e92d201eadec0deeeecac575f31","last_reissued_at":"2026-05-18T04:27:06.367471Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:27:06.367471Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dalitz plot analysis of Ds+ --> K+ K- pi+","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"P. del Amo Sanchez et al. (The BABAR Collaboration)","submitted_at":"2010-11-18T13:50:13Z","abstract_excerpt":"We perform a Dalitz plot analysis of about 100,000 Ds+ decays to K+ K- pi+ and measure the complex amplitudes of the intermediate resonances which contribute to this decay mode. We also measure the relative branching fractions of Ds+ --> K+ K+ pi- and Ds+ --> K+ K+ K-. For this analysis we use a 384 fb-1 data sample, recorded by the BABAR detector at the PEP-II asymmetric-energy e+e- collider running at center-of-mass energies near 10.58 GeV."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4190","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":""},"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":"1011.4190","created_at":"2026-05-18T04:27:06.367552+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.4190v2","created_at":"2026-05-18T04:27:06.367552+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4190","created_at":"2026-05-18T04:27:06.367552+00:00"},{"alias_kind":"pith_short_12","alias_value":"QZ5WP2LHBPBO","created_at":"2026-05-18T12:26:13.927090+00:00"},{"alias_kind":"pith_short_16","alias_value":"QZ5WP2LHBPBOJLOL","created_at":"2026-05-18T12:26:13.927090+00:00"},{"alias_kind":"pith_short_8","alias_value":"QZ5WP2LH","created_at":"2026-05-18T12:26:13.927090+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"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":96,"is_internal_anchor":true},{"citing_arxiv_id":"2506.15637","citing_title":"A covariant description of the interactions of axion-like particles and hadrons","ref_index":81,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS","json":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS.json","graph_json":"https://pith.science/api/pith-number/QZ5WP2LHBPBOJLOLLC7C3FLEAS/graph.json","events_json":"https://pith.science/api/pith-number/QZ5WP2LHBPBOJLOLLC7C3FLEAS/events.json","paper":"https://pith.science/paper/QZ5WP2LH"},"agent_actions":{"view_html":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS","download_json":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS.json","view_paper":"https://pith.science/paper/QZ5WP2LH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.4190&json=true","fetch_graph":"https://pith.science/api/pith-number/QZ5WP2LHBPBOJLOLLC7C3FLEAS/graph.json","fetch_events":"https://pith.science/api/pith-number/QZ5WP2LHBPBOJLOLLC7C3FLEAS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS/action/storage_attestation","attest_author":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS/action/author_attestation","sign_citation":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS/action/citation_signature","submit_replication":"https://pith.science/pith/QZ5WP2LHBPBOJLOLLC7C3FLEAS/action/replication_record"}},"created_at":"2026-05-18T04:27:06.367552+00:00","updated_at":"2026-05-18T04:27:06.367552+00:00"}