{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:C2J7TQ3Q6R46EEPDNF5CZDFJMP","short_pith_number":"pith:C2J7TQ3Q","schema_version":"1.0","canonical_sha256":"1693f9c370f479e211e3697a2c8ca963fd63a8843a5c68bed631ce380e3d8fdf","source":{"kind":"arxiv","id":"1807.06181","version":1},"attestation_state":"computed","paper":{"title":"Universal quark to gluon ratio in medium-induced parton cascade","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Soeren Schlichting, Yacine Mehtar-Tani","submitted_at":"2018-07-17T02:10:08Z","abstract_excerpt":"We investigate the radiative break-up of a highly energetic quark or gluon in a high-temperature QCD plasma. Within an inertial range of momenta $T \\ll \\omega \\ll E$, where $E$ denotes the energy of the original hard parton (jet) and $T$ the temperature of of the medium, we find that, as a result of the turbulent nature of the underlying parton cascade, the quark to gluon ratio of the soft fragments tends to a universal constant value that is independent of the initial conditions. We discuss implications of this result to jet quenching physics and the problem of thermalization of the quark-glu"},"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":"1807.06181","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-07-17T02:10:08Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"bac9b8e25edc5bf1dd433252e8fb9695c2e1bf4aef8e7a8a11c1850d781da21a","abstract_canon_sha256":"5356a47ea73f87cf8d6cb86bd547653bad82740de5053707aa58eaebd8fb4761"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:04.526094Z","signature_b64":"mzb9IH5DOuRSyyPavRMw7pWFz4SpbYQjCxdZsdZc46PjRycis3v0aLI/fCH3w/nJhZH6eOxF14fXNSGllAQtDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1693f9c370f479e211e3697a2c8ca963fd63a8843a5c68bed631ce380e3d8fdf","last_reissued_at":"2026-05-18T00:03:04.525493Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:04.525493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal quark to gluon ratio in medium-induced parton cascade","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Soeren Schlichting, Yacine Mehtar-Tani","submitted_at":"2018-07-17T02:10:08Z","abstract_excerpt":"We investigate the radiative break-up of a highly energetic quark or gluon in a high-temperature QCD plasma. Within an inertial range of momenta $T \\ll \\omega \\ll E$, where $E$ denotes the energy of the original hard parton (jet) and $T$ the temperature of of the medium, we find that, as a result of the turbulent nature of the underlying parton cascade, the quark to gluon ratio of the soft fragments tends to a universal constant value that is independent of the initial conditions. We discuss implications of this result to jet quenching physics and the problem of thermalization of the quark-glu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.06181","kind":"arxiv","version":1},"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":"1807.06181","created_at":"2026-05-18T00:03:04.525584+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.06181v1","created_at":"2026-05-18T00:03:04.525584+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.06181","created_at":"2026-05-18T00:03:04.525584+00:00"},{"alias_kind":"pith_short_12","alias_value":"C2J7TQ3Q6R46","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_16","alias_value":"C2J7TQ3Q6R46EEPD","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_8","alias_value":"C2J7TQ3Q","created_at":"2026-05-18T12:32:16.446611+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.25837","citing_title":"Deriving a parton shower for jet thermalization in QCD plasmas","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP","json":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP.json","graph_json":"https://pith.science/api/pith-number/C2J7TQ3Q6R46EEPDNF5CZDFJMP/graph.json","events_json":"https://pith.science/api/pith-number/C2J7TQ3Q6R46EEPDNF5CZDFJMP/events.json","paper":"https://pith.science/paper/C2J7TQ3Q"},"agent_actions":{"view_html":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP","download_json":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP.json","view_paper":"https://pith.science/paper/C2J7TQ3Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.06181&json=true","fetch_graph":"https://pith.science/api/pith-number/C2J7TQ3Q6R46EEPDNF5CZDFJMP/graph.json","fetch_events":"https://pith.science/api/pith-number/C2J7TQ3Q6R46EEPDNF5CZDFJMP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP/action/storage_attestation","attest_author":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP/action/author_attestation","sign_citation":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP/action/citation_signature","submit_replication":"https://pith.science/pith/C2J7TQ3Q6R46EEPDNF5CZDFJMP/action/replication_record"}},"created_at":"2026-05-18T00:03:04.525584+00:00","updated_at":"2026-05-18T00:03:04.525584+00:00"}