{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JP6SHYR6IRSY3QGIZFEZ47L4KH","short_pith_number":"pith:JP6SHYR6","schema_version":"1.0","canonical_sha256":"4bfd23e23e44658dc0c8c9499e7d7c51d043a7b4ec62bd812530df66bacd7c29","source":{"kind":"arxiv","id":"2411.16384","version":2},"attestation_state":"computed","paper":{"title":"How well does nonrelativistic QCD factorization work at next-to-leading order?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mathias Butenschoen, Nora Brambilla, Xiang-Peng Wang","submitted_at":"2024-11-25T13:44:40Z","abstract_excerpt":"We perform a thorough investigation of the universality of the long distance matrix elements (LDMEs) of nonrelativistic QCD factorization based on a next-to-leading order (NLO) fit of $J/\\psi$ color octet (CO) LDMEs to high transverse momentum $p_T$ $J/\\psi$ and $\\eta_c$ production data at the LHC. We thereby apply a novel fit-and-predict procedure to systematically take into account scale variations, and predict various observables never studied in this context before. In particular, the LDMEs can well describe $J/\\psi$ hadroproduction up to the highest measured values of $p_T$, as well as $\\"},"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":"2411.16384","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-25T13:44:40Z","cross_cats_sorted":[],"title_canon_sha256":"5889b96de058c5e3e259507902e45c5f1ab20cc7af24f9a5b49c36ad55d64c95","abstract_canon_sha256":"bf7d8a210778c4de60bd7dfec5613fe91610f99e518c65f1572451565f4280fd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:38:49.270422Z","signature_b64":"o7wUoYiFs5TyKgAYc2m+yt8Ou3dN7RN+IMKsehpYssifX5ZUTSl6qGjM9whsKkchjVhI674lgO78fIehFZFdAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4bfd23e23e44658dc0c8c9499e7d7c51d043a7b4ec62bd812530df66bacd7c29","last_reissued_at":"2026-07-05T11:38:49.269893Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:38:49.269893Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"How well does nonrelativistic QCD factorization work at next-to-leading order?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mathias Butenschoen, Nora Brambilla, Xiang-Peng Wang","submitted_at":"2024-11-25T13:44:40Z","abstract_excerpt":"We perform a thorough investigation of the universality of the long distance matrix elements (LDMEs) of nonrelativistic QCD factorization based on a next-to-leading order (NLO) fit of $J/\\psi$ color octet (CO) LDMEs to high transverse momentum $p_T$ $J/\\psi$ and $\\eta_c$ production data at the LHC. We thereby apply a novel fit-and-predict procedure to systematically take into account scale variations, and predict various observables never studied in this context before. In particular, the LDMEs can well describe $J/\\psi$ hadroproduction up to the highest measured values of $p_T$, as well as $\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.16384","kind":"arxiv","version":2},"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/2411.16384/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":"2411.16384","created_at":"2026-07-05T11:38:49.269951+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.16384v2","created_at":"2026-07-05T11:38:49.269951+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.16384","created_at":"2026-07-05T11:38:49.269951+00:00"},{"alias_kind":"pith_short_12","alias_value":"JP6SHYR6IRSY","created_at":"2026-07-05T11:38:49.269951+00:00"},{"alias_kind":"pith_short_16","alias_value":"JP6SHYR6IRSY3QGI","created_at":"2026-07-05T11:38:49.269951+00:00"},{"alias_kind":"pith_short_8","alias_value":"JP6SHYR6","created_at":"2026-07-05T11:38:49.269951+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.23594","citing_title":"Next-to-next-to-leading-order QCD corrections to ${}^3S_1^{(8)}$ gluon fragmentation function for quarkonium","ref_index":42,"is_internal_anchor":false},{"citing_arxiv_id":"2605.30441","citing_title":"Factorizing quarkonium production matrix elements using effective field theory","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2510.11809","citing_title":"Modeling the TMD shape function in $J/\\psi$ electroproduction","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH","json":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH.json","graph_json":"https://pith.science/api/pith-number/JP6SHYR6IRSY3QGIZFEZ47L4KH/graph.json","events_json":"https://pith.science/api/pith-number/JP6SHYR6IRSY3QGIZFEZ47L4KH/events.json","paper":"https://pith.science/paper/JP6SHYR6"},"agent_actions":{"view_html":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH","download_json":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH.json","view_paper":"https://pith.science/paper/JP6SHYR6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.16384&json=true","fetch_graph":"https://pith.science/api/pith-number/JP6SHYR6IRSY3QGIZFEZ47L4KH/graph.json","fetch_events":"https://pith.science/api/pith-number/JP6SHYR6IRSY3QGIZFEZ47L4KH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH/action/storage_attestation","attest_author":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH/action/author_attestation","sign_citation":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH/action/citation_signature","submit_replication":"https://pith.science/pith/JP6SHYR6IRSY3QGIZFEZ47L4KH/action/replication_record"}},"created_at":"2026-07-05T11:38:49.269951+00:00","updated_at":"2026-07-05T11:38:49.269951+00:00"}