{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:3JQFVFWK2FYH6SBA24ICIN6EJ2","short_pith_number":"pith:3JQFVFWK","schema_version":"1.0","canonical_sha256":"da605a96cad1707f4820d7102437c44eb64e5267783d78a25b56aeccc89367ce","source":{"kind":"arxiv","id":"hep-ph/0412060","version":3},"attestation_state":"computed","paper":{"title":"Multiple Parton Scattering in Nuclei: Heavy Quark Energy Loss and Modified Fragmentation Functions","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ben-Wei Zhang (IOPP), Enke Wang (IOPP & LBNL), Xin-Nian Wang (LBNL)","submitted_at":"2004-12-03T21:02:13Z","abstract_excerpt":"Multiple scattering, induced radiative energy loss and modified fragmentation functions of a heavy quark in nuclear matter are studied within the framework of generalized factorization in perturbative QCD. Modified heavy quark fragmentation functions and energy loss are derived in detail with illustration of the mass dependencies of the Landau-Pomeranchuk-Migdal interference effects and heavy quark energy loss. Due to the quark mass dependence of the gluon formation time, the nuclear size dependencies of nuclear modification of the heavy quark fragmentation function and heavy quark energy loss"},"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":"hep-ph/0412060","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-12-03T21:02:13Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"a3b977a813fc5fc069659f37aeaf565aadfbd373a0477babda80ab231ac6f9ba","abstract_canon_sha256":"93c6cb412a7b80619b44fecdc759edf8c2ae12e9858ab673a0b8e5b185ac5c9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:20.504960Z","signature_b64":"CPgLfuc9IwIYbpieQbxSn3XBpCMK32Q8QP4+IrBhSIThRxRDrVzeILOUlaxzpZAGD+8wOmp1aUvggROqYAIUBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da605a96cad1707f4820d7102437c44eb64e5267783d78a25b56aeccc89367ce","last_reissued_at":"2026-05-18T02:36:20.504286Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:20.504286Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multiple Parton Scattering in Nuclei: Heavy Quark Energy Loss and Modified Fragmentation Functions","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Ben-Wei Zhang (IOPP), Enke Wang (IOPP & LBNL), Xin-Nian Wang (LBNL)","submitted_at":"2004-12-03T21:02:13Z","abstract_excerpt":"Multiple scattering, induced radiative energy loss and modified fragmentation functions of a heavy quark in nuclear matter are studied within the framework of generalized factorization in perturbative QCD. Modified heavy quark fragmentation functions and energy loss are derived in detail with illustration of the mass dependencies of the Landau-Pomeranchuk-Migdal interference effects and heavy quark energy loss. Due to the quark mass dependence of the gluon formation time, the nuclear size dependencies of nuclear modification of the heavy quark fragmentation function and heavy quark energy loss"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0412060","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":""},"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":"hep-ph/0412060","created_at":"2026-05-18T02:36:20.504413+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0412060v3","created_at":"2026-05-18T02:36:20.504413+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0412060","created_at":"2026-05-18T02:36:20.504413+00:00"},{"alias_kind":"pith_short_12","alias_value":"3JQFVFWK2FYH","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"3JQFVFWK2FYH6SBA","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"3JQFVFWK","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"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":52,"is_internal_anchor":true},{"citing_arxiv_id":"2509.07842","citing_title":"Jet cone size dependence of single inclusive jet suppression due to jet quenching in Pb+Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","ref_index":79,"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":83,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2","json":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2.json","graph_json":"https://pith.science/api/pith-number/3JQFVFWK2FYH6SBA24ICIN6EJ2/graph.json","events_json":"https://pith.science/api/pith-number/3JQFVFWK2FYH6SBA24ICIN6EJ2/events.json","paper":"https://pith.science/paper/3JQFVFWK"},"agent_actions":{"view_html":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2","download_json":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2.json","view_paper":"https://pith.science/paper/3JQFVFWK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0412060&json=true","fetch_graph":"https://pith.science/api/pith-number/3JQFVFWK2FYH6SBA24ICIN6EJ2/graph.json","fetch_events":"https://pith.science/api/pith-number/3JQFVFWK2FYH6SBA24ICIN6EJ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2/action/storage_attestation","attest_author":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2/action/author_attestation","sign_citation":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2/action/citation_signature","submit_replication":"https://pith.science/pith/3JQFVFWK2FYH6SBA24ICIN6EJ2/action/replication_record"}},"created_at":"2026-05-18T02:36:20.504413+00:00","updated_at":"2026-05-18T02:36:20.504413+00:00"}