{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:P5WEPLJZYVSTW6HIJIFBBU2LCK","short_pith_number":"pith:P5WEPLJZ","schema_version":"1.0","canonical_sha256":"7f6c47ad39c5653b78e84a0a10d34b12879f84a285ce6b557f09244a06f29ac0","source":{"kind":"arxiv","id":"1911.10785","version":3},"attestation_state":"computed","paper":{"title":"Analysis of the semileptonic and nonleptonic two-body decays of the double heavy charm baryon states $\\Xi_{cc}^{++},\\,\\Xi_{cc}^{+}$ and $\\Omega_{cc}^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J\\\"urgen G. K\\\"orner, Mikhail A. Ivanov, Thomas Gutsche, Valery E. Lyubovitskij, Zhomart Tyulemissov","submitted_at":"2019-11-25T09:41:49Z","abstract_excerpt":"We calculate the semileptonic and a subclass of sixteen nonleptonic two-body decays of the double charm baryon ground states $\\Xi_{cc}^{++},\\,\\Xi_{cc}^{+}$ and $\\Omega_{cc}^+$ where we concentrate on the nonleptonic decay modes. We identify those nonleptonic decay channels in which the decay proceeds solely via the factorizing contribution precluding a contamination from $W$-exchange. We use the covariant confined quark model previously developed by us to calculate the various helicity amplitudes which describe the dynamics of the $1/2^+ \\to 1/2^+$ and $1/2^+ \\to 3/2^+$ transitions induced by "},"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":"1911.10785","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-11-25T09:41:49Z","cross_cats_sorted":[],"title_canon_sha256":"3ef2e3b7f1cc5cabf71f5d00ed4ac8c91df376deb04e493f729bf5305ff37627","abstract_canon_sha256":"91a1ce0bc4299046a496389cbe4d042aa996cbee553cebe9e673c5ea9ca2c4e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:27:59.328955Z","signature_b64":"pSe7DgHaGQBhr39HLCQUPsZQ6CIcF49lpoPUdSGh+FGK2o1AXQddw0RZx0dTVI/U+qFAqy/2BzCdPVkEqdBrDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f6c47ad39c5653b78e84a0a10d34b12879f84a285ce6b557f09244a06f29ac0","last_reissued_at":"2026-07-05T00:27:59.328481Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:27:59.328481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the semileptonic and nonleptonic two-body decays of the double heavy charm baryon states $\\Xi_{cc}^{++},\\,\\Xi_{cc}^{+}$ and $\\Omega_{cc}^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J\\\"urgen G. K\\\"orner, Mikhail A. Ivanov, Thomas Gutsche, Valery E. Lyubovitskij, Zhomart Tyulemissov","submitted_at":"2019-11-25T09:41:49Z","abstract_excerpt":"We calculate the semileptonic and a subclass of sixteen nonleptonic two-body decays of the double charm baryon ground states $\\Xi_{cc}^{++},\\,\\Xi_{cc}^{+}$ and $\\Omega_{cc}^+$ where we concentrate on the nonleptonic decay modes. We identify those nonleptonic decay channels in which the decay proceeds solely via the factorizing contribution precluding a contamination from $W$-exchange. We use the covariant confined quark model previously developed by us to calculate the various helicity amplitudes which describe the dynamics of the $1/2^+ \\to 1/2^+$ and $1/2^+ \\to 3/2^+$ transitions induced by "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.10785","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/1911.10785/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":"1911.10785","created_at":"2026-07-05T00:27:59.328539+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.10785v3","created_at":"2026-07-05T00:27:59.328539+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.10785","created_at":"2026-07-05T00:27:59.328539+00:00"},{"alias_kind":"pith_short_12","alias_value":"P5WEPLJZYVST","created_at":"2026-07-05T00:27:59.328539+00:00"},{"alias_kind":"pith_short_16","alias_value":"P5WEPLJZYVSTW6HI","created_at":"2026-07-05T00:27:59.328539+00:00"},{"alias_kind":"pith_short_8","alias_value":"P5WEPLJZ","created_at":"2026-07-05T00:27:59.328539+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/P5WEPLJZYVSTW6HIJIFBBU2LCK","json":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK.json","graph_json":"https://pith.science/api/pith-number/P5WEPLJZYVSTW6HIJIFBBU2LCK/graph.json","events_json":"https://pith.science/api/pith-number/P5WEPLJZYVSTW6HIJIFBBU2LCK/events.json","paper":"https://pith.science/paper/P5WEPLJZ"},"agent_actions":{"view_html":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK","download_json":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK.json","view_paper":"https://pith.science/paper/P5WEPLJZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.10785&json=true","fetch_graph":"https://pith.science/api/pith-number/P5WEPLJZYVSTW6HIJIFBBU2LCK/graph.json","fetch_events":"https://pith.science/api/pith-number/P5WEPLJZYVSTW6HIJIFBBU2LCK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK/action/storage_attestation","attest_author":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK/action/author_attestation","sign_citation":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK/action/citation_signature","submit_replication":"https://pith.science/pith/P5WEPLJZYVSTW6HIJIFBBU2LCK/action/replication_record"}},"created_at":"2026-07-05T00:27:59.328539+00:00","updated_at":"2026-07-05T00:27:59.328539+00:00"}