{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:CMODEWWYRYAN6ZU22KPZSK57CX","short_pith_number":"pith:CMODEWWY","schema_version":"1.0","canonical_sha256":"131c325ad88e00df669ad29f992bbf15f9e0c909d0ae59940b3bf890a45bd25b","source":{"kind":"arxiv","id":"nucl-th/0306027","version":3},"attestation_state":"computed","paper":{"title":"Hadron production in heavy ion collisions: Fragmentation and recombination from a dense parton phase","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"B. Muller, C. Nonaka, R.J.Fries, S.A. Bass","submitted_at":"2003-06-05T16:46:51Z","abstract_excerpt":"We discuss hadron production in heavy ion collisions at RHIC. We argue that hadrons at transverse momenta P_T < 5 GeV are formed by recombination of partons from the dense parton phase created in central collisions at RHIC. We provide a theoretical description of the recombination process for P_T > 2 GeV. Below P_T = 2 GeV our results smoothly match a purely statistical description. At high transverse momentum hadron production is well described in the language of perturbative QCD by the fragmentation of partons. We give numerical results for a variety of hadron spectra, ratios and nuclear sup"},"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/0306027","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2003-06-05T16:46:51Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"40fdc1037a7c766e1aefe15b6920ccf0e1dca858c5ee8563db5af7bd75ba4178","abstract_canon_sha256":"37b79e0cef6f92caa99ad18bfd2a4cf89fa6bfea21e54134bae0737c38d598d9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:35.205223Z","signature_b64":"y5jv0f7jvZPyLmQiObW6xfKol5Vf3/id2b85pE+OzgqcWZLXEjqHbBiSQ1ZWcco8WYbiWClZrgq216Vn1R0ABA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"131c325ad88e00df669ad29f992bbf15f9e0c909d0ae59940b3bf890a45bd25b","last_reissued_at":"2026-07-04T15:32:35.204804Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:35.204804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hadron production in heavy ion collisions: Fragmentation and recombination from a dense parton phase","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"B. Muller, C. Nonaka, R.J.Fries, S.A. Bass","submitted_at":"2003-06-05T16:46:51Z","abstract_excerpt":"We discuss hadron production in heavy ion collisions at RHIC. We argue that hadrons at transverse momenta P_T < 5 GeV are formed by recombination of partons from the dense parton phase created in central collisions at RHIC. We provide a theoretical description of the recombination process for P_T > 2 GeV. Below P_T = 2 GeV our results smoothly match a purely statistical description. At high transverse momentum hadron production is well described in the language of perturbative QCD by the fragmentation of partons. We give numerical results for a variety of hadron spectra, ratios and nuclear sup"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0306027","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/nucl-th/0306027/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/0306027","created_at":"2026-07-04T15:32:35.204864+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0306027v3","created_at":"2026-07-04T15:32:35.204864+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0306027","created_at":"2026-07-04T15:32:35.204864+00:00"},{"alias_kind":"pith_short_12","alias_value":"CMODEWWYRYAN","created_at":"2026-07-04T15:32:35.204864+00:00"},{"alias_kind":"pith_short_16","alias_value":"CMODEWWYRYAN6ZU2","created_at":"2026-07-04T15:32:35.204864+00:00"},{"alias_kind":"pith_short_8","alias_value":"CMODEWWY","created_at":"2026-07-04T15:32:35.204864+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2607.08707","citing_title":"Heavy quark coalescence probability in the presence of a potential","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2606.03552","citing_title":"$D^0$-$D_s^+$ Elliptic-Flow Splitting under Event-Shape Engineering: A Probe of Sequential Charm Hadronization","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2411.04969","citing_title":"Systematic study of flow of protons and light clusters in intermediate-energy heavy-ion collisions with momentum-dependent potentials","ref_index":83,"is_internal_anchor":true},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":14,"is_internal_anchor":true},{"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":90,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX","json":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX.json","graph_json":"https://pith.science/api/pith-number/CMODEWWYRYAN6ZU22KPZSK57CX/graph.json","events_json":"https://pith.science/api/pith-number/CMODEWWYRYAN6ZU22KPZSK57CX/events.json","paper":"https://pith.science/paper/CMODEWWY"},"agent_actions":{"view_html":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX","download_json":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX.json","view_paper":"https://pith.science/paper/CMODEWWY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0306027&json=true","fetch_graph":"https://pith.science/api/pith-number/CMODEWWYRYAN6ZU22KPZSK57CX/graph.json","fetch_events":"https://pith.science/api/pith-number/CMODEWWYRYAN6ZU22KPZSK57CX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX/action/storage_attestation","attest_author":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX/action/author_attestation","sign_citation":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX/action/citation_signature","submit_replication":"https://pith.science/pith/CMODEWWYRYAN6ZU22KPZSK57CX/action/replication_record"}},"created_at":"2026-07-04T15:32:35.204864+00:00","updated_at":"2026-07-04T15:32:35.204864+00:00"}