{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:BSV7JXDRZ4DFN2NEES7YJYCE4A","short_pith_number":"pith:BSV7JXDR","schema_version":"1.0","canonical_sha256":"0cabf4dc71cf0656e9a424bf84e044e022dcb8877279fb46230f539472965f9b","source":{"kind":"arxiv","id":"1911.08209","version":1},"attestation_state":"computed","paper":{"title":"Semileptonic decays of $D$ and $D_s$ mesons in the relativistic quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"R. N. Faustov, V. O. Galkin, Xian-Wei Kang","submitted_at":"2019-11-19T11:10:02Z","abstract_excerpt":"The form factors parameterizing the weak $D$ and $D_s$ transitions to light pseudoscalar and vector mesons are calculated in the framework of the relativistic quark model based on the quasipotential approach. The special attention is paid to the systematic account of the relativistic effects including transformation of the meson wave function from the rest to moving reference frame and contributions of the intermediate negative-energy states. The form factors are expressed through the overlap integrals of the meson wave functions, which are taken from previous studies of meson spectroscopy. Th"},"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":"1911.08209","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-11-19T11:10:02Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"1897cdc258e705ab80a8ca200bb252e87c799db801e65baccdf89ab6606e0068","abstract_canon_sha256":"b731981f34cd6d061b183094d5da84bdaaaa470ff49a67e357cdaa35fcd0d1e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:36:42.404945Z","signature_b64":"2uSQkTiXxYm89rVWPPAnTul6HIfFzu6LFFRImaKzNbIp8T1d9QqR5xbJyKq7ErHQs4AqTt5SNUEa1w1jdbFBBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0cabf4dc71cf0656e9a424bf84e044e022dcb8877279fb46230f539472965f9b","last_reissued_at":"2026-07-05T00:36:42.404514Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:36:42.404514Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Semileptonic decays of $D$ and $D_s$ mesons in the relativistic quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"R. N. Faustov, V. O. Galkin, Xian-Wei Kang","submitted_at":"2019-11-19T11:10:02Z","abstract_excerpt":"The form factors parameterizing the weak $D$ and $D_s$ transitions to light pseudoscalar and vector mesons are calculated in the framework of the relativistic quark model based on the quasipotential approach. The special attention is paid to the systematic account of the relativistic effects including transformation of the meson wave function from the rest to moving reference frame and contributions of the intermediate negative-energy states. The form factors are expressed through the overlap integrals of the meson wave functions, which are taken from previous studies of meson spectroscopy. Th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.08209","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/1911.08209/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":"1911.08209","created_at":"2026-07-05T00:36:42.404571+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.08209v1","created_at":"2026-07-05T00:36:42.404571+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.08209","created_at":"2026-07-05T00:36:42.404571+00:00"},{"alias_kind":"pith_short_12","alias_value":"BSV7JXDRZ4DF","created_at":"2026-07-05T00:36:42.404571+00:00"},{"alias_kind":"pith_short_16","alias_value":"BSV7JXDRZ4DFN2NE","created_at":"2026-07-05T00:36:42.404571+00:00"},{"alias_kind":"pith_short_8","alias_value":"BSV7JXDR","created_at":"2026-07-05T00:36:42.404571+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2511.14165","citing_title":"Systematic analysis of $D_{(s)}$ meson semi-leptonic decays in the covariant light-front quark model","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20644","citing_title":"Review of experimental studies of charmed meson decays at BESIII","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A","json":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A.json","graph_json":"https://pith.science/api/pith-number/BSV7JXDRZ4DFN2NEES7YJYCE4A/graph.json","events_json":"https://pith.science/api/pith-number/BSV7JXDRZ4DFN2NEES7YJYCE4A/events.json","paper":"https://pith.science/paper/BSV7JXDR"},"agent_actions":{"view_html":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A","download_json":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A.json","view_paper":"https://pith.science/paper/BSV7JXDR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.08209&json=true","fetch_graph":"https://pith.science/api/pith-number/BSV7JXDRZ4DFN2NEES7YJYCE4A/graph.json","fetch_events":"https://pith.science/api/pith-number/BSV7JXDRZ4DFN2NEES7YJYCE4A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A/action/storage_attestation","attest_author":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A/action/author_attestation","sign_citation":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A/action/citation_signature","submit_replication":"https://pith.science/pith/BSV7JXDRZ4DFN2NEES7YJYCE4A/action/replication_record"}},"created_at":"2026-07-05T00:36:42.404571+00:00","updated_at":"2026-07-05T00:36:42.404571+00:00"}