{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:HC5K4X52ND3ZCFOZCZNG6BFNNC","short_pith_number":"pith:HC5K4X52","schema_version":"1.0","canonical_sha256":"38baae5fba68f79115d9165a6f04ad68a947c5baa2ad51a2b4cce38ce2619f90","source":{"kind":"arxiv","id":"2206.09413","version":4},"attestation_state":"computed","paper":{"title":"The high-energy spectrum of QCD from inclusive emissions of charmed $B$-mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Francesco Giovanni Celiberto","submitted_at":"2022-06-19T14:36:32Z","abstract_excerpt":"We investigate the high-energy behavior of strong interactions through a study on the inclusive hadroproduction of charmed $B$-mesons ($B_c$ or $B_c^*$ states) accompanied by non-charmed $b$-hadron or light-flavored jet emissions at LHC energies and kinematic configurations. By making use of the hybrid high-energy and collinear factorization, where the standard fixed-order description based on collinear parton densities and fragmentation functions is enhanced via the Balitsky-Fadin-Kuraev-Lipatov (BFKL) resummation of energy logarithms, we perform a full next-to-leading order analysis of distr"},"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":"2206.09413","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-06-19T14:36:32Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6566df28082a56dea9f6466843a6b2b094ad37b41bf91c17ed83e190c43aec72","abstract_canon_sha256":"c94bf10852db8bc1e71565885c96e72d2d7a65fcaa59091c6bb4d48e161a8ca7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:17:27.317790Z","signature_b64":"/mdMVESd7c19XsoqcDftbvhPPOhMHWR6iAQcBYj8D+uiajhurRXZrMgoe903QDwQaCVlBDU72n0o0HrbECzCCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38baae5fba68f79115d9165a6f04ad68a947c5baa2ad51a2b4cce38ce2619f90","last_reissued_at":"2026-07-05T05:17:27.317276Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:17:27.317276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The high-energy spectrum of QCD from inclusive emissions of charmed $B$-mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Francesco Giovanni Celiberto","submitted_at":"2022-06-19T14:36:32Z","abstract_excerpt":"We investigate the high-energy behavior of strong interactions through a study on the inclusive hadroproduction of charmed $B$-mesons ($B_c$ or $B_c^*$ states) accompanied by non-charmed $b$-hadron or light-flavored jet emissions at LHC energies and kinematic configurations. By making use of the hybrid high-energy and collinear factorization, where the standard fixed-order description based on collinear parton densities and fragmentation functions is enhanced via the Balitsky-Fadin-Kuraev-Lipatov (BFKL) resummation of energy logarithms, we perform a full next-to-leading order analysis of distr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.09413","kind":"arxiv","version":4},"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/2206.09413/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":"2206.09413","created_at":"2026-07-05T05:17:27.317356+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.09413v4","created_at":"2026-07-05T05:17:27.317356+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.09413","created_at":"2026-07-05T05:17:27.317356+00:00"},{"alias_kind":"pith_short_12","alias_value":"HC5K4X52ND3Z","created_at":"2026-07-05T05:17:27.317356+00:00"},{"alias_kind":"pith_short_16","alias_value":"HC5K4X52ND3ZCFOZ","created_at":"2026-07-05T05:17:27.317356+00:00"},{"alias_kind":"pith_short_8","alias_value":"HC5K4X52","created_at":"2026-07-05T05:17:27.317356+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.20063","citing_title":"Toward Precision Fragmentation of $\\Omega_{3Q}$ Baryons: The OMG3Q1.1 Framework","ref_index":120,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01539","citing_title":"Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron Colliders","ref_index":136,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11646","citing_title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","ref_index":166,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC","json":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC.json","graph_json":"https://pith.science/api/pith-number/HC5K4X52ND3ZCFOZCZNG6BFNNC/graph.json","events_json":"https://pith.science/api/pith-number/HC5K4X52ND3ZCFOZCZNG6BFNNC/events.json","paper":"https://pith.science/paper/HC5K4X52"},"agent_actions":{"view_html":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC","download_json":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC.json","view_paper":"https://pith.science/paper/HC5K4X52","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.09413&json=true","fetch_graph":"https://pith.science/api/pith-number/HC5K4X52ND3ZCFOZCZNG6BFNNC/graph.json","fetch_events":"https://pith.science/api/pith-number/HC5K4X52ND3ZCFOZCZNG6BFNNC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC/action/storage_attestation","attest_author":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC/action/author_attestation","sign_citation":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC/action/citation_signature","submit_replication":"https://pith.science/pith/HC5K4X52ND3ZCFOZCZNG6BFNNC/action/replication_record"}},"created_at":"2026-07-05T05:17:27.317356+00:00","updated_at":"2026-07-05T05:17:27.317356+00:00"}