{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:33PWUJWBORNVV2GEAMOFNXWP3V","short_pith_number":"pith:33PWUJWB","schema_version":"1.0","canonical_sha256":"dedf6a26c1745b5ae8c4031c56decfdd784b4cfcfa3599d93d21b59649621562","source":{"kind":"arxiv","id":"1509.05907","version":2},"attestation_state":"computed","paper":{"title":"QCD factorization for high $p_T$ heavy quarkonium production","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"George Sterman, Hong Zhang, Jian-Wei Qiu, Yan-Qing Ma","submitted_at":"2015-09-19T15:49:18Z","abstract_excerpt":"In this talk, we present the QCD factorization formula for heavy quarkonium production at large $p_T$ with factorized leading-power and next-to-leading power contributions in the $1/p_T$ expansion. We show that the leading order analytical calculations in this QCD factorization approach can reproduce effectively the full next-to-leading order numerical results derived using non-relativistic QCD (NRQCD) factorization formalism. We demonstrate that the next-to-leading power contributions are crucial to the description of the channels that are the most relevant for the rate as well as polarizatio"},"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":"1509.05907","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-19T15:49:18Z","cross_cats_sorted":[],"title_canon_sha256":"3a7d3220774b1c0dc1b2a7d9c25f4cd581d34a4335791880a521b3f0ec75d8b9","abstract_canon_sha256":"72c656e8a520997c3c4d6b5430673d836c374a496fc1fd13e1b0e0828a91d493"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:57.088464Z","signature_b64":"8xqh93XYix9TwyrblusYgnqvCaMRFm7OqcYetHxNpftXoPdBDI+ks0r1CfmFrFLWstz2RrD0taCGD6DSDd4HCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dedf6a26c1745b5ae8c4031c56decfdd784b4cfcfa3599d93d21b59649621562","last_reissued_at":"2026-05-18T01:25:57.087869Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:57.087869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD factorization for high $p_T$ heavy quarkonium production","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"George Sterman, Hong Zhang, Jian-Wei Qiu, Yan-Qing Ma","submitted_at":"2015-09-19T15:49:18Z","abstract_excerpt":"In this talk, we present the QCD factorization formula for heavy quarkonium production at large $p_T$ with factorized leading-power and next-to-leading power contributions in the $1/p_T$ expansion. We show that the leading order analytical calculations in this QCD factorization approach can reproduce effectively the full next-to-leading order numerical results derived using non-relativistic QCD (NRQCD) factorization formalism. We demonstrate that the next-to-leading power contributions are crucial to the description of the channels that are the most relevant for the rate as well as polarizatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.05907","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":""},"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":"1509.05907","created_at":"2026-05-18T01:25:57.087958+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.05907v2","created_at":"2026-05-18T01:25:57.087958+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.05907","created_at":"2026-05-18T01:25:57.087958+00:00"},{"alias_kind":"pith_short_12","alias_value":"33PWUJWBORNV","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"33PWUJWBORNVV2GE","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"33PWUJWB","created_at":"2026-05-18T12:29:02.477457+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/33PWUJWBORNVV2GEAMOFNXWP3V","json":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V.json","graph_json":"https://pith.science/api/pith-number/33PWUJWBORNVV2GEAMOFNXWP3V/graph.json","events_json":"https://pith.science/api/pith-number/33PWUJWBORNVV2GEAMOFNXWP3V/events.json","paper":"https://pith.science/paper/33PWUJWB"},"agent_actions":{"view_html":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V","download_json":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V.json","view_paper":"https://pith.science/paper/33PWUJWB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.05907&json=true","fetch_graph":"https://pith.science/api/pith-number/33PWUJWBORNVV2GEAMOFNXWP3V/graph.json","fetch_events":"https://pith.science/api/pith-number/33PWUJWBORNVV2GEAMOFNXWP3V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V/action/storage_attestation","attest_author":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V/action/author_attestation","sign_citation":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V/action/citation_signature","submit_replication":"https://pith.science/pith/33PWUJWBORNVV2GEAMOFNXWP3V/action/replication_record"}},"created_at":"2026-05-18T01:25:57.087958+00:00","updated_at":"2026-05-18T01:25:57.087958+00:00"}