{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:ACMTQL7FCV6MUBWPQOFK4FQPJL","short_pith_number":"pith:ACMTQL7F","schema_version":"1.0","canonical_sha256":"0099382fe5157cca06cf838aae160f4af010d4bec02412e680f76711ebe8091e","source":{"kind":"arxiv","id":"2005.10832","version":1},"attestation_state":"computed","paper":{"title":"Exploring $J/\\psi$ production mechanism at the future Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hongxi Xing, Jian-Wei Qiu, Xiang-Peng Wang","submitted_at":"2020-05-21T18:00:00Z","abstract_excerpt":"We propose to use transverse momentum $p_T$ distribution of $J/\\psi$ production at the future Electron Ion Collider (EIC) to explore the production mechanism of heavy quarkonia in high energy collisions. We apply QCD and QED collinear factorization to the production of a $c\\bar{c}$ pair at high $p_T$, and non-relativistic QCD factorization to the hadronization of the pair to a $J/\\psi$. We evaluate $J/\\psi$ $p_T$-distribution at both leading and next-to-leading order in strong coupling, and show that production rates for various color-spin channels of a $c\\bar{c}$ pair in electron-hadron colli"},"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":"2005.10832","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-05-21T18:00:00Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"b2815beb9081d2a35804a1f9f19c01e6b1d405c74c10d48147fd8b1e36d2f27f","abstract_canon_sha256":"484084b0967832dd3e07e03abaf734630b003a13c18509ec906f7ae239d8b099"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:55:30.375702Z","signature_b64":"6iNHskNlNoCqhGpIvLwodRRHEWIf868g03oE9HxUwZwpi2VaeArkhGCuyDf0lHKcBPrqqCM2JvUspgY+KftsAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0099382fe5157cca06cf838aae160f4af010d4bec02412e680f76711ebe8091e","last_reissued_at":"2026-07-05T02:55:30.375293Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:55:30.375293Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring $J/\\psi$ production mechanism at the future Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hongxi Xing, Jian-Wei Qiu, Xiang-Peng Wang","submitted_at":"2020-05-21T18:00:00Z","abstract_excerpt":"We propose to use transverse momentum $p_T$ distribution of $J/\\psi$ production at the future Electron Ion Collider (EIC) to explore the production mechanism of heavy quarkonia in high energy collisions. We apply QCD and QED collinear factorization to the production of a $c\\bar{c}$ pair at high $p_T$, and non-relativistic QCD factorization to the hadronization of the pair to a $J/\\psi$. We evaluate $J/\\psi$ $p_T$-distribution at both leading and next-to-leading order in strong coupling, and show that production rates for various color-spin channels of a $c\\bar{c}$ pair in electron-hadron colli"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.10832","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/2005.10832/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":"2005.10832","created_at":"2026-07-05T02:55:30.375362+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.10832v1","created_at":"2026-07-05T02:55:30.375362+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.10832","created_at":"2026-07-05T02:55:30.375362+00:00"},{"alias_kind":"pith_short_12","alias_value":"ACMTQL7FCV6M","created_at":"2026-07-05T02:55:30.375362+00:00"},{"alias_kind":"pith_short_16","alias_value":"ACMTQL7FCV6MUBWP","created_at":"2026-07-05T02:55:30.375362+00:00"},{"alias_kind":"pith_short_8","alias_value":"ACMTQL7F","created_at":"2026-07-05T02:55:30.375362+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07664","citing_title":"Single inclusive hadron and jet production in lepton-hadron scattering","ref_index":26,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL","json":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL.json","graph_json":"https://pith.science/api/pith-number/ACMTQL7FCV6MUBWPQOFK4FQPJL/graph.json","events_json":"https://pith.science/api/pith-number/ACMTQL7FCV6MUBWPQOFK4FQPJL/events.json","paper":"https://pith.science/paper/ACMTQL7F"},"agent_actions":{"view_html":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL","download_json":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL.json","view_paper":"https://pith.science/paper/ACMTQL7F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.10832&json=true","fetch_graph":"https://pith.science/api/pith-number/ACMTQL7FCV6MUBWPQOFK4FQPJL/graph.json","fetch_events":"https://pith.science/api/pith-number/ACMTQL7FCV6MUBWPQOFK4FQPJL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL/action/storage_attestation","attest_author":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL/action/author_attestation","sign_citation":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL/action/citation_signature","submit_replication":"https://pith.science/pith/ACMTQL7FCV6MUBWPQOFK4FQPJL/action/replication_record"}},"created_at":"2026-07-05T02:55:30.375362+00:00","updated_at":"2026-07-05T02:55:30.375362+00:00"}