{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:D337YN7C5LRSGNYVULYNJMZSL6","short_pith_number":"pith:D337YN7C","schema_version":"1.0","canonical_sha256":"1ef7fc37e2eae3233715a2f0d4b3325faeed31cd615ed7ad0cb436347fa2677c","source":{"kind":"arxiv","id":"nucl-ex/0601033","version":2},"attestation_state":"computed","paper":{"title":"Identified hadron spectra at large transverse momentum in p+p and d+Au collisions at \\sqrts_NN = 200 GeV","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"nucl-ex","authors_text":"STAR Collaboration","submitted_at":"2006-01-24T15:03:50Z","abstract_excerpt":"We present the transverse momentum (pT) spectra for identified charged pions, protons and anti-protons from p+p and d+Au collisions at \\sqrts_NN = 200 GeV. The spectra are measured around midrapidity (|y| < 0.5) over the range of 0.3 < pT < 10 GeV/c with particle identification from the ionization energy loss and its relativistic rise in the Time Projection Chamber and Time-of-Flight in STAR. The charged pion and proton+anti-proton spectra at high pT in p+p and d+Au collisions are in good agreement with a phenomenological model (EPOS) and with the next-to-leading order perturbative quantum chr"},"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":"nucl-ex/0601033","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2006-01-24T15:03:50Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"1546816622eeb2b715bd7131cc989550312f505bc4699a46330fb8206b55ea2f","abstract_canon_sha256":"6fcf6f4421b7d6cd65158a4707afc6560dad877650a104776fe916f133c9e82c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:09.951429Z","signature_b64":"gUar1M3hKezs5lQvNLFrzxhzpSt21oxh5bdEdQ3wys9lhSfMIo7+xXRhM7akpYIgHHnh9ESUh4nHTMHAwTlgCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ef7fc37e2eae3233715a2f0d4b3325faeed31cd615ed7ad0cb436347fa2677c","last_reissued_at":"2026-05-18T03:47:09.950968Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:09.950968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Identified hadron spectra at large transverse momentum in p+p and d+Au collisions at \\sqrts_NN = 200 GeV","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"nucl-ex","authors_text":"STAR Collaboration","submitted_at":"2006-01-24T15:03:50Z","abstract_excerpt":"We present the transverse momentum (pT) spectra for identified charged pions, protons and anti-protons from p+p and d+Au collisions at \\sqrts_NN = 200 GeV. The spectra are measured around midrapidity (|y| < 0.5) over the range of 0.3 < pT < 10 GeV/c with particle identification from the ionization energy loss and its relativistic rise in the Time Projection Chamber and Time-of-Flight in STAR. The charged pion and proton+anti-proton spectra at high pT in p+p and d+Au collisions are in good agreement with a phenomenological model (EPOS) and with the next-to-leading order perturbative quantum chr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0601033","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":"nucl-ex/0601033","created_at":"2026-05-18T03:47:09.951038+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0601033v2","created_at":"2026-05-18T03:47:09.951038+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0601033","created_at":"2026-05-18T03:47:09.951038+00:00"},{"alias_kind":"pith_short_12","alias_value":"D337YN7C5LRS","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"D337YN7C5LRSGNYV","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"D337YN7C","created_at":"2026-05-18T12:25:53.939244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.08830","citing_title":"Nuclear parton distributions and nuclear shadowing","ref_index":139,"is_internal_anchor":true},{"citing_arxiv_id":"2506.17454","citing_title":"Nuclear Cold QCD: Review and Future Strategy","ref_index":219,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6","json":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6.json","graph_json":"https://pith.science/api/pith-number/D337YN7C5LRSGNYVULYNJMZSL6/graph.json","events_json":"https://pith.science/api/pith-number/D337YN7C5LRSGNYVULYNJMZSL6/events.json","paper":"https://pith.science/paper/D337YN7C"},"agent_actions":{"view_html":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6","download_json":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6.json","view_paper":"https://pith.science/paper/D337YN7C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0601033&json=true","fetch_graph":"https://pith.science/api/pith-number/D337YN7C5LRSGNYVULYNJMZSL6/graph.json","fetch_events":"https://pith.science/api/pith-number/D337YN7C5LRSGNYVULYNJMZSL6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6/action/storage_attestation","attest_author":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6/action/author_attestation","sign_citation":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6/action/citation_signature","submit_replication":"https://pith.science/pith/D337YN7C5LRSGNYVULYNJMZSL6/action/replication_record"}},"created_at":"2026-05-18T03:47:09.951038+00:00","updated_at":"2026-05-18T03:47:09.951038+00:00"}