{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:V6PVTSDXFHYRHSPM6XTUIDMLG6","short_pith_number":"pith:V6PVTSDX","schema_version":"1.0","canonical_sha256":"af9f59c87729f113c9ecf5e7440d8b379f9dcbc19cfa2f8a05a4aa51d123cbf9","source":{"kind":"arxiv","id":"1311.3005","version":1},"attestation_state":"computed","paper":{"title":"Universal attractor in a highly occupied non-Abelian plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Juergen Berges, Kirill Boguslavski, Raju Venugopalan, Soeren Schlichting","submitted_at":"2013-11-13T02:59:10Z","abstract_excerpt":"We study the thermalization process in highly occupied non-Abelian plasmas at weak coupling. The non-equilibrium dynamics of such systems is classical in nature and can be simulated with real-time lattice gauge theory techniques. We provide a detailed discussion of this framework and elaborate on the results reported in~\\cite{Berges:2013eia} along with novel findings. We demonstrate the emergence of universal attractor solutions, which govern the non-equilibrium evolution on large time scales both for non-expanding and expanding non-Abelian plasmas. The turbulent attractor for a non-expanding "},"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":"1311.3005","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-13T02:59:10Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"4e31c2d39fd72ba06c19e147fb36bec652c8c13cc7ef981996dde366d0a4d5f9","abstract_canon_sha256":"bc2ff5e30868ee48cac91580e18b4a9b941505d0f3b450f7adc4ad2b8e248722"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:03.143252Z","signature_b64":"yFbPaGrs7210s/1wLG18YHvE5pug4b5EtE3PyF+tt1StvOXdt2PLnQbmzioQiQGwfSxn3LxlTvoitrim7qdvCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af9f59c87729f113c9ecf5e7440d8b379f9dcbc19cfa2f8a05a4aa51d123cbf9","last_reissued_at":"2026-05-18T02:50:03.142478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:03.142478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal attractor in a highly occupied non-Abelian plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Juergen Berges, Kirill Boguslavski, Raju Venugopalan, Soeren Schlichting","submitted_at":"2013-11-13T02:59:10Z","abstract_excerpt":"We study the thermalization process in highly occupied non-Abelian plasmas at weak coupling. The non-equilibrium dynamics of such systems is classical in nature and can be simulated with real-time lattice gauge theory techniques. We provide a detailed discussion of this framework and elaborate on the results reported in~\\cite{Berges:2013eia} along with novel findings. We demonstrate the emergence of universal attractor solutions, which govern the non-equilibrium evolution on large time scales both for non-expanding and expanding non-Abelian plasmas. The turbulent attractor for a non-expanding "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3005","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":"1311.3005","created_at":"2026-05-18T02:50:03.142612+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.3005v1","created_at":"2026-05-18T02:50:03.142612+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3005","created_at":"2026-05-18T02:50:03.142612+00:00"},{"alias_kind":"pith_short_12","alias_value":"V6PVTSDXFHYR","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"V6PVTSDXFHYRHSPM","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"V6PVTSDX","created_at":"2026-05-18T12:28:04.890932+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.25669","citing_title":"Minijet thermalization and jet transport coefficients in QCD kinetic theory","ref_index":90,"is_internal_anchor":true},{"citing_arxiv_id":"2604.08520","citing_title":"Kinetic and canonical momentum broadening in the Glasma","ref_index":108,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07256","citing_title":"Revisiting the sphaleron and axion production rates in QCD at high temperatures","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07256","citing_title":"Revisiting the sphaleron and axion production rates in QCD at high temperatures","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6","json":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6.json","graph_json":"https://pith.science/api/pith-number/V6PVTSDXFHYRHSPM6XTUIDMLG6/graph.json","events_json":"https://pith.science/api/pith-number/V6PVTSDXFHYRHSPM6XTUIDMLG6/events.json","paper":"https://pith.science/paper/V6PVTSDX"},"agent_actions":{"view_html":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6","download_json":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6.json","view_paper":"https://pith.science/paper/V6PVTSDX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.3005&json=true","fetch_graph":"https://pith.science/api/pith-number/V6PVTSDXFHYRHSPM6XTUIDMLG6/graph.json","fetch_events":"https://pith.science/api/pith-number/V6PVTSDXFHYRHSPM6XTUIDMLG6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6/action/storage_attestation","attest_author":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6/action/author_attestation","sign_citation":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6/action/citation_signature","submit_replication":"https://pith.science/pith/V6PVTSDXFHYRHSPM6XTUIDMLG6/action/replication_record"}},"created_at":"2026-05-18T02:50:03.142612+00:00","updated_at":"2026-05-18T02:50:03.142612+00:00"}