{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:3GVWNFA53QMBBHPJO5RYYKAODR","short_pith_number":"pith:3GVWNFA5","schema_version":"1.0","canonical_sha256":"d9ab66941ddc18109de977638c280e1c60874dfa9bfbc5c1d747c9c0e25c4c88","source":{"kind":"arxiv","id":"hep-ph/0504019","version":3},"attestation_state":"computed","paper":{"title":"The High-Temperature Phase of Landau-Gauge Yang-Mills Theory","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Axel Maas, Jochen Wambach, Reinhard Alkofer","submitted_at":"2005-04-04T12:37:26Z","abstract_excerpt":"The properties of the high-temperature phase of Yang-Mills theory in Landau gauge are investigated by extending an earlier study on the infinite-temperature limit to finite temperatures. To this end the Dyson-Schwinger equations for the propagators of the gluon and the Faddeev-Popov ghost are solved analytically in the infrared and numerically at non-vanishing momenta. Gluons, polarized transversely with respect to the heat bath are found to comply with the Gribov-Zwanziger and the Kugo-Ojima scenario, while longitudinally polarized gluons are screened. Therefore the high-temperature phase is "},"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/0504019","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-04T12:37:26Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"45c4545e4033e507c9f190b7156fb00a41903ee22b2f9801df7da85dea01f9fa","abstract_canon_sha256":"1ef4148a69a07e671e95c186183a168c2eb6028a9823d3612fadcc82f77610f6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:27.650561Z","signature_b64":"RlXOWuu+tbPajEI1Z0E7Zd8jA3VopSlBQS9sEppcrYAxSPddQV4SVS7T+BUMlj9ykQAa7G08AKrxsn1YmmNgAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9ab66941ddc18109de977638c280e1c60874dfa9bfbc5c1d747c9c0e25c4c88","last_reissued_at":"2026-05-18T04:13:27.649928Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:27.649928Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The High-Temperature Phase of Landau-Gauge Yang-Mills Theory","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Axel Maas, Jochen Wambach, Reinhard Alkofer","submitted_at":"2005-04-04T12:37:26Z","abstract_excerpt":"The properties of the high-temperature phase of Yang-Mills theory in Landau gauge are investigated by extending an earlier study on the infinite-temperature limit to finite temperatures. To this end the Dyson-Schwinger equations for the propagators of the gluon and the Faddeev-Popov ghost are solved analytically in the infrared and numerically at non-vanishing momenta. Gluons, polarized transversely with respect to the heat bath are found to comply with the Gribov-Zwanziger and the Kugo-Ojima scenario, while longitudinally polarized gluons are screened. Therefore the high-temperature phase is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0504019","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/0504019","created_at":"2026-05-18T04:13:27.650029+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0504019v3","created_at":"2026-05-18T04:13:27.650029+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0504019","created_at":"2026-05-18T04:13:27.650029+00:00"},{"alias_kind":"pith_short_12","alias_value":"3GVWNFA53QMB","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"3GVWNFA53QMBBHPJ","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"3GVWNFA5","created_at":"2026-05-18T12:25:52.687210+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR","json":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR.json","graph_json":"https://pith.science/api/pith-number/3GVWNFA53QMBBHPJO5RYYKAODR/graph.json","events_json":"https://pith.science/api/pith-number/3GVWNFA53QMBBHPJO5RYYKAODR/events.json","paper":"https://pith.science/paper/3GVWNFA5"},"agent_actions":{"view_html":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR","download_json":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR.json","view_paper":"https://pith.science/paper/3GVWNFA5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0504019&json=true","fetch_graph":"https://pith.science/api/pith-number/3GVWNFA53QMBBHPJO5RYYKAODR/graph.json","fetch_events":"https://pith.science/api/pith-number/3GVWNFA53QMBBHPJO5RYYKAODR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR/action/storage_attestation","attest_author":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR/action/author_attestation","sign_citation":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR/action/citation_signature","submit_replication":"https://pith.science/pith/3GVWNFA53QMBBHPJO5RYYKAODR/action/replication_record"}},"created_at":"2026-05-18T04:13:27.650029+00:00","updated_at":"2026-05-18T04:13:27.650029+00:00"}