{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1991:GSVGH7WOIN7G5DYJXREUZ3SA4F","short_pith_number":"pith:GSVGH7WO","schema_version":"1.0","canonical_sha256":"34aa63fece437e6e8f09bc494cee40e15dc0cbcfb928a1df6194d2d7633dd465","source":{"kind":"arxiv","id":"hep-th/9109051","version":1},"attestation_state":"computed","paper":{"title":"The Damping of Energetic Gluons and Quarks in High-Temperature QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.L. Marini, C.P. Burgess","submitted_at":"1991-09-26T15:08:39Z","abstract_excerpt":"When a gluon or a quark is sent through the hot QCD plasma it can be absorbed into the ambient heat bath and so can acquire an effective lifetime. At high temperatures and for weak couplings the inverse lifetime, or damping rate, for energetic quarks and transverse gluons, (those whose momenta satisfy $|\\p| \\gg gT$) is given by $\\gamma(\\p) = c\\; g^2 \\log\\left({1\\over g}\\right)\\; T + O(g^2T)$. We show that very simple arguments suffice both to fix the numerical coefficient, $c$, in this expression and to show that the $O(g^2T)$ contribution is incalculable in perturbation theory without further"},"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-th/9109051","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1991-09-26T15:08:39Z","cross_cats_sorted":[],"title_canon_sha256":"c90a34fba3c439b96b80dc830013cfd47f986c075df12c5cf373910d7bdb1c55","abstract_canon_sha256":"eb42f58b4dcfde173e859c6445ebc5ac9461e60a1166e29bef727380706daf7c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:18:28.420450Z","signature_b64":"A2myNSjrHvbj7EU47aFOVnywLYsRCtI9/dNApmh9I9l2F7UMUOTUCxOKsONGvnS1Tq5ZNSRCiaddmUJjA4DoBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"34aa63fece437e6e8f09bc494cee40e15dc0cbcfb928a1df6194d2d7633dd465","last_reissued_at":"2026-07-04T17:18:28.420102Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:18:28.420102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Damping of Energetic Gluons and Quarks in High-Temperature QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.L. Marini, C.P. Burgess","submitted_at":"1991-09-26T15:08:39Z","abstract_excerpt":"When a gluon or a quark is sent through the hot QCD plasma it can be absorbed into the ambient heat bath and so can acquire an effective lifetime. At high temperatures and for weak couplings the inverse lifetime, or damping rate, for energetic quarks and transverse gluons, (those whose momenta satisfy $|\\p| \\gg gT$) is given by $\\gamma(\\p) = c\\; g^2 \\log\\left({1\\over g}\\right)\\; T + O(g^2T)$. We show that very simple arguments suffice both to fix the numerical coefficient, $c$, in this expression and to show that the $O(g^2T)$ contribution is incalculable in perturbation theory without further"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9109051","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9109051/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":"hep-th/9109051","created_at":"2026-07-04T17:18:28.420158+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9109051v1","created_at":"2026-07-04T17:18:28.420158+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9109051","created_at":"2026-07-04T17:18:28.420158+00:00"},{"alias_kind":"pith_short_12","alias_value":"GSVGH7WOIN7G","created_at":"2026-07-04T17:18:28.420158+00:00"},{"alias_kind":"pith_short_16","alias_value":"GSVGH7WOIN7G5DYJ","created_at":"2026-07-04T17:18:28.420158+00:00"},{"alias_kind":"pith_short_8","alias_value":"GSVGH7WO","created_at":"2026-07-04T17:18:28.420158+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.07961","citing_title":"Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F","json":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F.json","graph_json":"https://pith.science/api/pith-number/GSVGH7WOIN7G5DYJXREUZ3SA4F/graph.json","events_json":"https://pith.science/api/pith-number/GSVGH7WOIN7G5DYJXREUZ3SA4F/events.json","paper":"https://pith.science/paper/GSVGH7WO"},"agent_actions":{"view_html":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F","download_json":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F.json","view_paper":"https://pith.science/paper/GSVGH7WO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9109051&json=true","fetch_graph":"https://pith.science/api/pith-number/GSVGH7WOIN7G5DYJXREUZ3SA4F/graph.json","fetch_events":"https://pith.science/api/pith-number/GSVGH7WOIN7G5DYJXREUZ3SA4F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F/action/storage_attestation","attest_author":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F/action/author_attestation","sign_citation":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F/action/citation_signature","submit_replication":"https://pith.science/pith/GSVGH7WOIN7G5DYJXREUZ3SA4F/action/replication_record"}},"created_at":"2026-07-04T17:18:28.420158+00:00","updated_at":"2026-07-04T17:18:28.420158+00:00"}