{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:SJBWLVDPS2ESWVSEB7V5HM7B5K","short_pith_number":"pith:SJBWLVDP","schema_version":"1.0","canonical_sha256":"924365d46f96892b56440febd3b3e1eaa92a6a17aa66ccb5e2ff9409e182dead","source":{"kind":"arxiv","id":"hep-ph/0102230","version":2},"attestation_state":"computed","paper":{"title":"Multiple Parton Scattering in Nuclei: Parton Energy Loss","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Xiaofeng Guo, Xin-Nian Wang","submitted_at":"2001-02-19T08:12:18Z","abstract_excerpt":"Multiple parton scattering and induced parton energy loss is studied in deeply inelastic scattering (DIS) off nuclei. The effect of multiple scattering of a highly off-shell quark and the induced parton energy loss is expressed in terms of the modification to the quark fragmentation functions. We derive such modified quark fragmentation functions and their QCD evolution equations in DIS using generalized factorization of higher twist parton distributions. We consider double-hard, hard-soft parton scattering as well as their interferences in the same framework. The final result, which depends o"},"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/0102230","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-02-19T08:12:18Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"8e349973fde1b632d3523ac6904bd9ee1b654c58bb256b4df4c7c40ef11c00d9","abstract_canon_sha256":"f810a815cd76146d44355f83bf3e17b8428cf373d6043d0ed70d10f66cbdef22"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:48.137654Z","signature_b64":"Qa3xETiNagcsD1IbBfhbRCF/hFQMIjUg4lSLzJQhZuS/UvnDf0dNs+gglAET01Mn8OcTzHjg/FKnRwgMEYPqAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"924365d46f96892b56440febd3b3e1eaa92a6a17aa66ccb5e2ff9409e182dead","last_reissued_at":"2026-05-18T02:36:48.137045Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:48.137045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multiple Parton Scattering in Nuclei: Parton Energy Loss","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Xiaofeng Guo, Xin-Nian Wang","submitted_at":"2001-02-19T08:12:18Z","abstract_excerpt":"Multiple parton scattering and induced parton energy loss is studied in deeply inelastic scattering (DIS) off nuclei. The effect of multiple scattering of a highly off-shell quark and the induced parton energy loss is expressed in terms of the modification to the quark fragmentation functions. We derive such modified quark fragmentation functions and their QCD evolution equations in DIS using generalized factorization of higher twist parton distributions. We consider double-hard, hard-soft parton scattering as well as their interferences in the same framework. The final result, which depends o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0102230","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":"hep-ph/0102230","created_at":"2026-05-18T02:36:48.137155+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0102230v2","created_at":"2026-05-18T02:36:48.137155+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0102230","created_at":"2026-05-18T02:36:48.137155+00:00"},{"alias_kind":"pith_short_12","alias_value":"SJBWLVDPS2ES","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"SJBWLVDPS2ESWVSE","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"SJBWLVDP","created_at":"2026-05-18T12:25:50.845339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"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":65,"is_internal_anchor":true},{"citing_arxiv_id":"2509.10743","citing_title":"Glauber quark and gluon contributions to quark energy loss at next-to-leading order and next-to-leading twist","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2512.12959","citing_title":"Energy Loss of a Heavy Quark in a Collisional Quark-Gluon Plasma","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K","json":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K.json","graph_json":"https://pith.science/api/pith-number/SJBWLVDPS2ESWVSEB7V5HM7B5K/graph.json","events_json":"https://pith.science/api/pith-number/SJBWLVDPS2ESWVSEB7V5HM7B5K/events.json","paper":"https://pith.science/paper/SJBWLVDP"},"agent_actions":{"view_html":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K","download_json":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K.json","view_paper":"https://pith.science/paper/SJBWLVDP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0102230&json=true","fetch_graph":"https://pith.science/api/pith-number/SJBWLVDPS2ESWVSEB7V5HM7B5K/graph.json","fetch_events":"https://pith.science/api/pith-number/SJBWLVDPS2ESWVSEB7V5HM7B5K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K/action/storage_attestation","attest_author":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K/action/author_attestation","sign_citation":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K/action/citation_signature","submit_replication":"https://pith.science/pith/SJBWLVDPS2ESWVSEB7V5HM7B5K/action/replication_record"}},"created_at":"2026-05-18T02:36:48.137155+00:00","updated_at":"2026-05-18T02:36:48.137155+00:00"}