{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:YI6YJCTUVYF5ADDETNLD5JMLB2","short_pith_number":"pith:YI6YJCTU","schema_version":"1.0","canonical_sha256":"c23d848a74ae0bd00c649b563ea58b0e8e0dfe9cc2ff14d0a4d514c0207256a6","source":{"kind":"arxiv","id":"hep-ph/9508406","version":1},"attestation_state":"computed","paper":{"title":"On the Convergence of Perturbative QCD at High Temperature","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agustin Nieto, Eric Braaten","submitted_at":"1995-08-30T21:54:08Z","abstract_excerpt":"The free energy for QCD at high temperature $T$ is calculated to order $g^5$ using effective-field-theory methods to separate the contributions from the momentum scales $T$ and $gT$. The effects of the scale $T$ enter through the coefficients in the effective lagrangian for the 3-dimensional effective theory obtained by dimensional reduction. The perturbation series for these coefficients seem to be well-behaved if the running coupling constant is sufficiently small: $\\alpha_s(2 \\pi T) \\ll 1$. For the contribution to the free energy from the scale $gT$, the perturbation series is well-behaved "},"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/9508406","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-30T21:54:08Z","cross_cats_sorted":[],"title_canon_sha256":"815cadda8e6f87368771992d54a25ed40596a705ce52dceebaca093b1a7b44af","abstract_canon_sha256":"ab50e97a3a921a5481a446339c4239cbae9ef3be207143021151e96e865b6be2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:05.805909Z","signature_b64":"R4/OhKPMyL7qDBFVg5QHueS/4SDVMPHicj/2bzMY4Gs8Jh16KO9y++2yKw9hRf+Ptgd/PqZzaBJpQ4/soD5kBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c23d848a74ae0bd00c649b563ea58b0e8e0dfe9cc2ff14d0a4d514c0207256a6","last_reissued_at":"2026-05-18T01:08:05.805254Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:05.805254Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the Convergence of Perturbative QCD at High Temperature","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Agustin Nieto, Eric Braaten","submitted_at":"1995-08-30T21:54:08Z","abstract_excerpt":"The free energy for QCD at high temperature $T$ is calculated to order $g^5$ using effective-field-theory methods to separate the contributions from the momentum scales $T$ and $gT$. The effects of the scale $T$ enter through the coefficients in the effective lagrangian for the 3-dimensional effective theory obtained by dimensional reduction. The perturbation series for these coefficients seem to be well-behaved if the running coupling constant is sufficiently small: $\\alpha_s(2 \\pi T) \\ll 1$. For the contribution to the free energy from the scale $gT$, the perturbation series is well-behaved "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9508406","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":"hep-ph/9508406","created_at":"2026-05-18T01:08:05.805363+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9508406v1","created_at":"2026-05-18T01:08:05.805363+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9508406","created_at":"2026-05-18T01:08:05.805363+00:00"},{"alias_kind":"pith_short_12","alias_value":"YI6YJCTUVYF5","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"YI6YJCTUVYF5ADDE","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"YI6YJCTU","created_at":"2026-05-18T12:25:47.700082+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/YI6YJCTUVYF5ADDETNLD5JMLB2","json":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2.json","graph_json":"https://pith.science/api/pith-number/YI6YJCTUVYF5ADDETNLD5JMLB2/graph.json","events_json":"https://pith.science/api/pith-number/YI6YJCTUVYF5ADDETNLD5JMLB2/events.json","paper":"https://pith.science/paper/YI6YJCTU"},"agent_actions":{"view_html":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2","download_json":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2.json","view_paper":"https://pith.science/paper/YI6YJCTU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9508406&json=true","fetch_graph":"https://pith.science/api/pith-number/YI6YJCTUVYF5ADDETNLD5JMLB2/graph.json","fetch_events":"https://pith.science/api/pith-number/YI6YJCTUVYF5ADDETNLD5JMLB2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2/action/storage_attestation","attest_author":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2/action/author_attestation","sign_citation":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2/action/citation_signature","submit_replication":"https://pith.science/pith/YI6YJCTUVYF5ADDETNLD5JMLB2/action/replication_record"}},"created_at":"2026-05-18T01:08:05.805363+00:00","updated_at":"2026-05-18T01:08:05.805363+00:00"}