{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:RH2MNETZALX2LFPVF4DCD7YXKJ","short_pith_number":"pith:RH2MNETZ","schema_version":"1.0","canonical_sha256":"89f4c6927902efa595f52f0621ff17524f6f9bb136a86045a19b6befd102c35b","source":{"kind":"arxiv","id":"2211.11780","version":1},"attestation_state":"computed","paper":{"title":"Stabilizing BFKL via heavy-flavor and NRQCD fragmentation","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":"2022-11-21T19:00:02Z","abstract_excerpt":"We bring evidence that the recently discovered property of natural stability of the high-energy resummation is directly connected to the fragmentation mechanism of heavy hadrons. As a phenomenological support, we provide predictions for differential distributions sensitive to heavy-hadron tags, calculated at the next-to-leading logarithmic level of the hybrid high-energy/collinear factorization (NLL/NLO), as implemented in the JETHAD multimodular code. We show that the stabilizing mechanism is encoded in gluon channels of both heavy-flavor collinear fragmentation functions extracted from data "},"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":"2211.11780","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-11-21T19:00:02Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"a063d4aae8a0f8755e935d995f24d32e1bf68677cb4ed0a4051c45c78719934a","abstract_canon_sha256":"62cad54c6d612180131424883624cbc0c616e611436ddd498516fc20e2b61eab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:18:09.358496Z","signature_b64":"1J4p6rWgaFkpypUaEVGO1ZVYAjKbkzdmUyY2sFi7tQlItYF1NnL0ZBwXGmgLGk6DdDCM59Jp9K0ngfYKa7BYCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89f4c6927902efa595f52f0621ff17524f6f9bb136a86045a19b6befd102c35b","last_reissued_at":"2026-07-05T05:18:09.358073Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:18:09.358073Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stabilizing BFKL via heavy-flavor and NRQCD fragmentation","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":"2022-11-21T19:00:02Z","abstract_excerpt":"We bring evidence that the recently discovered property of natural stability of the high-energy resummation is directly connected to the fragmentation mechanism of heavy hadrons. As a phenomenological support, we provide predictions for differential distributions sensitive to heavy-hadron tags, calculated at the next-to-leading logarithmic level of the hybrid high-energy/collinear factorization (NLL/NLO), as implemented in the JETHAD multimodular code. We show that the stabilizing mechanism is encoded in gluon channels of both heavy-flavor collinear fragmentation functions extracted from data "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.11780","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/2211.11780/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":"2211.11780","created_at":"2026-07-05T05:18:09.358143+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.11780v1","created_at":"2026-07-05T05:18:09.358143+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.11780","created_at":"2026-07-05T05:18:09.358143+00:00"},{"alias_kind":"pith_short_12","alias_value":"RH2MNETZALX2","created_at":"2026-07-05T05:18:09.358143+00:00"},{"alias_kind":"pith_short_16","alias_value":"RH2MNETZALX2LFPV","created_at":"2026-07-05T05:18:09.358143+00:00"},{"alias_kind":"pith_short_8","alias_value":"RH2MNETZ","created_at":"2026-07-05T05:18:09.358143+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":224,"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":202,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11646","citing_title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","ref_index":224,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ","json":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ.json","graph_json":"https://pith.science/api/pith-number/RH2MNETZALX2LFPVF4DCD7YXKJ/graph.json","events_json":"https://pith.science/api/pith-number/RH2MNETZALX2LFPVF4DCD7YXKJ/events.json","paper":"https://pith.science/paper/RH2MNETZ"},"agent_actions":{"view_html":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ","download_json":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ.json","view_paper":"https://pith.science/paper/RH2MNETZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.11780&json=true","fetch_graph":"https://pith.science/api/pith-number/RH2MNETZALX2LFPVF4DCD7YXKJ/graph.json","fetch_events":"https://pith.science/api/pith-number/RH2MNETZALX2LFPVF4DCD7YXKJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ/action/storage_attestation","attest_author":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ/action/author_attestation","sign_citation":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ/action/citation_signature","submit_replication":"https://pith.science/pith/RH2MNETZALX2LFPVF4DCD7YXKJ/action/replication_record"}},"created_at":"2026-07-05T05:18:09.358143+00:00","updated_at":"2026-07-05T05:18:09.358143+00:00"}