{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:AZI3APCZ366FAUZKXWGIQLJJ4L","short_pith_number":"pith:AZI3APCZ","schema_version":"1.0","canonical_sha256":"0651b03c59dfbc50532abd8c882d29e2ef6d2b866c6a505d936a68f72147b09f","source":{"kind":"arxiv","id":"nucl-th/0211010","version":2},"attestation_state":"computed","paper":{"title":"Scaling behavior at high p_T and the p/pi ratio","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C.B. Yang, Rudolph C. Hwa","submitted_at":"2002-11-05T17:16:28Z","abstract_excerpt":"We first show that the pions produced at high $p_T$ in heavy-ion collisions over a wide range of high energies exhibit a scaling behavior when the distributions are plotted in terms of a scaling variable. We then use the recombination model to calculate the scaling quark distribution just before hadronization. From the quark distribution it is then possible to calculate the proton distribution at high $p_T$, also in the framework of the recombination model. The resultant $p/\\pi$ ratio exceeds one in the intermediate $p_T$ region where data exist, but the scaling result for the proton distribut"},"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-th/0211010","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2002-11-05T17:16:28Z","cross_cats_sorted":[],"title_canon_sha256":"dd5097466382fb6f215f582b3b2761af1739670c3b3dfba6b75a2529f14a3022","abstract_canon_sha256":"5590374fd9e40938f9bbe56759e7f4bb9a30ca8055c1e3dd6934d54dc0f61c27"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:35:33.569621Z","signature_b64":"NjPlMfklr0YQ8hXaakzkLqvbwVOdXKYCx+T5Qv5nufokLbTQb1l0p/msFNEH0cs6nxd0LxKXJxMMp2guXIV9Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0651b03c59dfbc50532abd8c882d29e2ef6d2b866c6a505d936a68f72147b09f","last_reissued_at":"2026-07-04T16:35:33.569101Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:35:33.569101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scaling behavior at high p_T and the p/pi ratio","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C.B. Yang, Rudolph C. Hwa","submitted_at":"2002-11-05T17:16:28Z","abstract_excerpt":"We first show that the pions produced at high $p_T$ in heavy-ion collisions over a wide range of high energies exhibit a scaling behavior when the distributions are plotted in terms of a scaling variable. We then use the recombination model to calculate the scaling quark distribution just before hadronization. From the quark distribution it is then possible to calculate the proton distribution at high $p_T$, also in the framework of the recombination model. The resultant $p/\\pi$ ratio exceeds one in the intermediate $p_T$ region where data exist, but the scaling result for the proton distribut"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0211010","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/nucl-th/0211010/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":"nucl-th/0211010","created_at":"2026-07-04T16:35:33.569181+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0211010v2","created_at":"2026-07-04T16:35:33.569181+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0211010","created_at":"2026-07-04T16:35:33.569181+00:00"},{"alias_kind":"pith_short_12","alias_value":"AZI3APCZ366F","created_at":"2026-07-04T16:35:33.569181+00:00"},{"alias_kind":"pith_short_16","alias_value":"AZI3APCZ366FAUZK","created_at":"2026-07-04T16:35:33.569181+00:00"},{"alias_kind":"pith_short_8","alias_value":"AZI3APCZ","created_at":"2026-07-04T16:35:33.569181+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":88,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01762","citing_title":"Transverse momentum dependence of $\\Omega/\\phi$ ratio in high energy collisions","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L","json":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L.json","graph_json":"https://pith.science/api/pith-number/AZI3APCZ366FAUZKXWGIQLJJ4L/graph.json","events_json":"https://pith.science/api/pith-number/AZI3APCZ366FAUZKXWGIQLJJ4L/events.json","paper":"https://pith.science/paper/AZI3APCZ"},"agent_actions":{"view_html":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L","download_json":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L.json","view_paper":"https://pith.science/paper/AZI3APCZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0211010&json=true","fetch_graph":"https://pith.science/api/pith-number/AZI3APCZ366FAUZKXWGIQLJJ4L/graph.json","fetch_events":"https://pith.science/api/pith-number/AZI3APCZ366FAUZKXWGIQLJJ4L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L/action/storage_attestation","attest_author":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L/action/author_attestation","sign_citation":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L/action/citation_signature","submit_replication":"https://pith.science/pith/AZI3APCZ366FAUZKXWGIQLJJ4L/action/replication_record"}},"created_at":"2026-07-04T16:35:33.569181+00:00","updated_at":"2026-07-04T16:35:33.569181+00:00"}