{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:PFOGVIK6Y5XJY56XKM3Q46K76T","short_pith_number":"pith:PFOGVIK6","schema_version":"1.0","canonical_sha256":"795c6aa15ec76e9c77d753370e795ff4f1b938ce40d46b718a84dc0b6043f55f","source":{"kind":"arxiv","id":"nucl-th/0703019","version":3},"attestation_state":"computed","paper":{"title":"Jet modification in three dimensional fluid dynamics at next-to-leading twist","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Majumder, C. Nonaka, S. A. Bass","submitted_at":"2007-03-07T20:59:33Z","abstract_excerpt":"The modification of the single inclusive spectrum of high transverse momentum ($p_T $) pions emanating from an ultra-relativistic heavy-ion collision is investigated. The deconfined sector is modelled using a full three dimensional (3-D) ideal fluid dynamics simulation. Energy loss of high $p_T$ partons and the ensuing modification of their fragmentation is calculated within perturbative QCD at next-to-leading twist, where the magnitude of the higher twist contribution is modulated by the entropy density extracted from the 3-D fluid dynamics simulation. The nuclear modification factor ($R_{AA}"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"nucl-th/0703019","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2007-03-07T20:59:33Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"1bf65265aa6c2f0d193d37f87f93a0cf15272a67e2661d9bff411c14db860049","abstract_canon_sha256":"d4a6c4ee5c26e47679ecd4b6991192506068c06b1e581ad123cb972d006d01d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:25:25.582402Z","signature_b64":"XFdXpGIVKm7C3OsB5gzzvUSEHJeCp7/BomwX4kNsqBNAz9gXwSFCaHlIt3xdBWzVUqHNlAEmtutK4YdfwWjjBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"795c6aa15ec76e9c77d753370e795ff4f1b938ce40d46b718a84dc0b6043f55f","last_reissued_at":"2026-07-04T15:25:25.581942Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:25:25.581942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet modification in three dimensional fluid dynamics at next-to-leading twist","license":"","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Majumder, C. Nonaka, S. A. Bass","submitted_at":"2007-03-07T20:59:33Z","abstract_excerpt":"The modification of the single inclusive spectrum of high transverse momentum ($p_T $) pions emanating from an ultra-relativistic heavy-ion collision is investigated. The deconfined sector is modelled using a full three dimensional (3-D) ideal fluid dynamics simulation. Energy loss of high $p_T$ partons and the ensuing modification of their fragmentation is calculated within perturbative QCD at next-to-leading twist, where the magnitude of the higher twist contribution is modulated by the entropy density extracted from the 3-D fluid dynamics simulation. The nuclear modification factor ($R_{AA}"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0703019","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/0703019/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/0703019","created_at":"2026-07-04T15:25:25.582001+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0703019v3","created_at":"2026-07-04T15:25:25.582001+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0703019","created_at":"2026-07-04T15:25:25.582001+00:00"},{"alias_kind":"pith_short_12","alias_value":"PFOGVIK6Y5XJ","created_at":"2026-07-04T15:25:25.582001+00:00"},{"alias_kind":"pith_short_16","alias_value":"PFOGVIK6Y5XJY56X","created_at":"2026-07-04T15:25:25.582001+00:00"},{"alias_kind":"pith_short_8","alias_value":"PFOGVIK6","created_at":"2026-07-04T15:25:25.582001+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/PFOGVIK6Y5XJY56XKM3Q46K76T","json":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T.json","graph_json":"https://pith.science/api/pith-number/PFOGVIK6Y5XJY56XKM3Q46K76T/graph.json","events_json":"https://pith.science/api/pith-number/PFOGVIK6Y5XJY56XKM3Q46K76T/events.json","paper":"https://pith.science/paper/PFOGVIK6"},"agent_actions":{"view_html":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T","download_json":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T.json","view_paper":"https://pith.science/paper/PFOGVIK6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0703019&json=true","fetch_graph":"https://pith.science/api/pith-number/PFOGVIK6Y5XJY56XKM3Q46K76T/graph.json","fetch_events":"https://pith.science/api/pith-number/PFOGVIK6Y5XJY56XKM3Q46K76T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T/action/storage_attestation","attest_author":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T/action/author_attestation","sign_citation":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T/action/citation_signature","submit_replication":"https://pith.science/pith/PFOGVIK6Y5XJY56XKM3Q46K76T/action/replication_record"}},"created_at":"2026-07-04T15:25:25.582001+00:00","updated_at":"2026-07-04T15:25:25.582001+00:00"}