{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:KEN5HKLOD7DLVI5APIRLR3VFKV","short_pith_number":"pith:KEN5HKLO","schema_version":"1.0","canonical_sha256":"511bd3a96e1fc6baa3a07a22b8eea5554233e185314737703e23287b63f8a3e7","source":{"kind":"arxiv","id":"hep-ph/0103169","version":1},"attestation_state":"computed","paper":{"title":"Baryons with two heavy quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.K.Likhoded, V.V.Kiselev","submitted_at":"2001-03-15T07:15:48Z","abstract_excerpt":"We consider general physical characteristics of doubly heavy baryons: the spectroscopy in the framework of potential approach and sum rules of QCD, mechanisms of production in various interactions on the basis of fragmentation model with account of preasymptotic corrections caused by higher twists over the transverse momentum of baryon, inclusive decays and lifetimes in the operator product expansion over the inverse powers of heavy quark masses as well as the exclusive decays in the sum rules of QCD. We generalize the methods developed in the effective theory of heavy quarks towards the descr"},"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":"hep-ph/0103169","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-15T07:15:48Z","cross_cats_sorted":[],"title_canon_sha256":"3ed44328ceb0e6ccb81e4dd8bfa6a7d8661820cad23f751586069de92928fd82","abstract_canon_sha256":"a68210eb8d8ba200ace7521db9ba63f3c6e906cc803cd523353aa0e0d1fb81ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:05.254373Z","signature_b64":"k6yvGpXQccWRbd7JJNCubx9dY9uNqx4JBp9asMifURTxZV2I7hTIrWlEVKWzWhQEFOUq2ZlTM34xi8Mh4CrRDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"511bd3a96e1fc6baa3a07a22b8eea5554233e185314737703e23287b63f8a3e7","last_reissued_at":"2026-05-18T04:33:05.253801Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:05.253801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryons with two heavy quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.K.Likhoded, V.V.Kiselev","submitted_at":"2001-03-15T07:15:48Z","abstract_excerpt":"We consider general physical characteristics of doubly heavy baryons: the spectroscopy in the framework of potential approach and sum rules of QCD, mechanisms of production in various interactions on the basis of fragmentation model with account of preasymptotic corrections caused by higher twists over the transverse momentum of baryon, inclusive decays and lifetimes in the operator product expansion over the inverse powers of heavy quark masses as well as the exclusive decays in the sum rules of QCD. We generalize the methods developed in the effective theory of heavy quarks towards the descr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0103169","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":"hep-ph/0103169","created_at":"2026-05-18T04:33:05.253914+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0103169v1","created_at":"2026-05-18T04:33:05.253914+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0103169","created_at":"2026-05-18T04:33:05.253914+00:00"},{"alias_kind":"pith_short_12","alias_value":"KEN5HKLOD7DL","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"KEN5HKLOD7DLVI5A","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"KEN5HKLO","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2305.02243","citing_title":"Revisiting lifetimes of doubly charmed baryons","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2601.07015","citing_title":"Light cone QCD sum rules study of the rare radiative $\\Xi^{*}_{bb}\\to\\Xi_b\\gamma$ decay","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2603.01037","citing_title":"Quark-diquark effective mass formalism for heavy baryon spectroscopy","ref_index":104,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04967","citing_title":"New Predictions for the Lifetimes of Doubly Heavy Baryons and the $B_c$ Meson","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10939","citing_title":"Study of doubly heavy baryon lifetimes","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV","json":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV.json","graph_json":"https://pith.science/api/pith-number/KEN5HKLOD7DLVI5APIRLR3VFKV/graph.json","events_json":"https://pith.science/api/pith-number/KEN5HKLOD7DLVI5APIRLR3VFKV/events.json","paper":"https://pith.science/paper/KEN5HKLO"},"agent_actions":{"view_html":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV","download_json":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV.json","view_paper":"https://pith.science/paper/KEN5HKLO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0103169&json=true","fetch_graph":"https://pith.science/api/pith-number/KEN5HKLOD7DLVI5APIRLR3VFKV/graph.json","fetch_events":"https://pith.science/api/pith-number/KEN5HKLOD7DLVI5APIRLR3VFKV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV/action/storage_attestation","attest_author":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV/action/author_attestation","sign_citation":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV/action/citation_signature","submit_replication":"https://pith.science/pith/KEN5HKLOD7DLVI5APIRLR3VFKV/action/replication_record"}},"created_at":"2026-05-18T04:33:05.253914+00:00","updated_at":"2026-05-18T04:33:05.253914+00:00"}