{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:TBYMWII475XMU7DJRQ2OJFZP4H","short_pith_number":"pith:TBYMWII4","schema_version":"1.0","canonical_sha256":"9870cb211cff6eca7c698c34e4972fe1c5b1d8bdcddd6652e70a697bd9e884bc","source":{"kind":"arxiv","id":"2112.06789","version":3},"attestation_state":"computed","paper":{"title":"Matching next-to-leading-order and high-energy-resummed calculations of heavy-quarkonium-hadroproduction cross sections","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jean-Philippe Lansberg, Maxim Nefedov, Melih A. Ozcelik","submitted_at":"2021-12-13T16:51:45Z","abstract_excerpt":"The energy dependence of the total hadroproduction cross section of pseudo-scalar quarkonia is computed via matching Next-to-Leading Order (NLO) Collinear-Factorisation (CF) results with resummed higher-order corrections, proportional to $\\alpha_s^{n}\\ln^{n-1}(1/z)$, to the CF hard-scattering coefficient, where $z=M^2/\\hat{s}$ with $M$ and $\\hat{s}$ being the quarkonium mass and the partonic center-of-mass energy squared. The resummation is performed using High-Energy Factorisation (HEF) in the Doubly-Logarithmic (DL) approximation, which is a subset of the leading logarithmic $\\ln (1/z)$ appr"},"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":"2112.06789","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-13T16:51:45Z","cross_cats_sorted":[],"title_canon_sha256":"fb825404f11048106155578bd7e54e19aeb2a0c7d8cd39d2a701804de1655868","abstract_canon_sha256":"41f9b50f2aa76cd19a95b17644e4505c6bd1fb498f10950fcf9d9ad58b3cad9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:34:48.870377Z","signature_b64":"8erdDrOFQkANruHzyubQIMBRxrssrS6AUhBUD/e7HEEk7hZZTFobCGTSLAw1UoV+CP6kZ9EAApCR5AA4RN0lAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9870cb211cff6eca7c698c34e4972fe1c5b1d8bdcddd6652e70a697bd9e884bc","last_reissued_at":"2026-07-05T04:34:48.869899Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:34:48.869899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Matching next-to-leading-order and high-energy-resummed calculations of heavy-quarkonium-hadroproduction cross sections","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jean-Philippe Lansberg, Maxim Nefedov, Melih A. Ozcelik","submitted_at":"2021-12-13T16:51:45Z","abstract_excerpt":"The energy dependence of the total hadroproduction cross section of pseudo-scalar quarkonia is computed via matching Next-to-Leading Order (NLO) Collinear-Factorisation (CF) results with resummed higher-order corrections, proportional to $\\alpha_s^{n}\\ln^{n-1}(1/z)$, to the CF hard-scattering coefficient, where $z=M^2/\\hat{s}$ with $M$ and $\\hat{s}$ being the quarkonium mass and the partonic center-of-mass energy squared. The resummation is performed using High-Energy Factorisation (HEF) in the Doubly-Logarithmic (DL) approximation, which is a subset of the leading logarithmic $\\ln (1/z)$ appr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.06789","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/2112.06789/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":"2112.06789","created_at":"2026-07-05T04:34:48.869955+00:00"},{"alias_kind":"arxiv_version","alias_value":"2112.06789v3","created_at":"2026-07-05T04:34:48.869955+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.06789","created_at":"2026-07-05T04:34:48.869955+00:00"},{"alias_kind":"pith_short_12","alias_value":"TBYMWII475XM","created_at":"2026-07-05T04:34:48.869955+00:00"},{"alias_kind":"pith_short_16","alias_value":"TBYMWII475XMU7DJ","created_at":"2026-07-05T04:34:48.869955+00:00"},{"alias_kind":"pith_short_8","alias_value":"TBYMWII4","created_at":"2026-07-05T04:34:48.869955+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/TBYMWII475XMU7DJRQ2OJFZP4H","json":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H.json","graph_json":"https://pith.science/api/pith-number/TBYMWII475XMU7DJRQ2OJFZP4H/graph.json","events_json":"https://pith.science/api/pith-number/TBYMWII475XMU7DJRQ2OJFZP4H/events.json","paper":"https://pith.science/paper/TBYMWII4"},"agent_actions":{"view_html":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H","download_json":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H.json","view_paper":"https://pith.science/paper/TBYMWII4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2112.06789&json=true","fetch_graph":"https://pith.science/api/pith-number/TBYMWII475XMU7DJRQ2OJFZP4H/graph.json","fetch_events":"https://pith.science/api/pith-number/TBYMWII475XMU7DJRQ2OJFZP4H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H/action/storage_attestation","attest_author":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H/action/author_attestation","sign_citation":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H/action/citation_signature","submit_replication":"https://pith.science/pith/TBYMWII475XMU7DJRQ2OJFZP4H/action/replication_record"}},"created_at":"2026-07-05T04:34:48.869955+00:00","updated_at":"2026-07-05T04:34:48.869955+00:00"}