{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:V3ZVJCVOA55NDZJKWIYZ2AZWKA","short_pith_number":"pith:V3ZVJCVO","schema_version":"1.0","canonical_sha256":"aef3548aae077ad1e52ab2319d03365030f388dc6baab4ab03eaca1da1f7451b","source":{"kind":"arxiv","id":"1708.03482","version":2},"attestation_state":"computed","paper":{"title":"Non-perturbative finite-temperature Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Anton K. Cyrol, Jan M. Pawlowski, Mario Mitter, Nils Strodthoff","submitted_at":"2017-08-11T09:26:51Z","abstract_excerpt":"We present non-perturbative correlation functions in Landau-gauge Yang-Mills theory at finite temperature. The results are obtained from the functional renormalisation group within a self-consistent approximation scheme. In particular, we compute the magnetic and electric components of the gluon propagator, and the three- and four-gluon vertices. We also show the ghost propagator and the ghost-gluon vertex at finite temperature. Our results for the propagators are confronted with lattice simulations and our Debye mass is compared to hard thermal loop perturbation theory."},"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":"1708.03482","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-11T09:26:51Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"7c8fe3c144849e7dd4a6afa766c7eea0d5fed111820b5b48eb749412b0234b61","abstract_canon_sha256":"7129d2e7956b762b47a285a5f24c18fb14cd16f59329ad0ab436a1c4ef52de98"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:20:46.834647Z","signature_b64":"oHdfoDwDKvjGqn20KhqRDT8llSPwVX+i8Gprgbf3rDVjWtnycuyPEld5AfWHg5lwNuts4WOb4X8PvJob9z0kAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aef3548aae077ad1e52ab2319d03365030f388dc6baab4ab03eaca1da1f7451b","last_reissued_at":"2026-05-18T00:20:46.832812Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:20:46.832812Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbative finite-temperature Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Anton K. Cyrol, Jan M. Pawlowski, Mario Mitter, Nils Strodthoff","submitted_at":"2017-08-11T09:26:51Z","abstract_excerpt":"We present non-perturbative correlation functions in Landau-gauge Yang-Mills theory at finite temperature. The results are obtained from the functional renormalisation group within a self-consistent approximation scheme. In particular, we compute the magnetic and electric components of the gluon propagator, and the three- and four-gluon vertices. We also show the ghost propagator and the ghost-gluon vertex at finite temperature. Our results for the propagators are confronted with lattice simulations and our Debye mass is compared to hard thermal loop perturbation theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.03482","kind":"arxiv","version":2},"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":"1708.03482","created_at":"2026-05-18T00:20:46.834092+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.03482v2","created_at":"2026-05-18T00:20:46.834092+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.03482","created_at":"2026-05-18T00:20:46.834092+00:00"},{"alias_kind":"pith_short_12","alias_value":"V3ZVJCVOA55N","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"V3ZVJCVOA55NDZJK","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"V3ZVJCVO","created_at":"2026-05-18T12:31:49.984773+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.08435","citing_title":"Emergence of dynamical tensor fields in composite models of gravity","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA","json":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA.json","graph_json":"https://pith.science/api/pith-number/V3ZVJCVOA55NDZJKWIYZ2AZWKA/graph.json","events_json":"https://pith.science/api/pith-number/V3ZVJCVOA55NDZJKWIYZ2AZWKA/events.json","paper":"https://pith.science/paper/V3ZVJCVO"},"agent_actions":{"view_html":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA","download_json":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA.json","view_paper":"https://pith.science/paper/V3ZVJCVO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.03482&json=true","fetch_graph":"https://pith.science/api/pith-number/V3ZVJCVOA55NDZJKWIYZ2AZWKA/graph.json","fetch_events":"https://pith.science/api/pith-number/V3ZVJCVOA55NDZJKWIYZ2AZWKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA/action/storage_attestation","attest_author":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA/action/author_attestation","sign_citation":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA/action/citation_signature","submit_replication":"https://pith.science/pith/V3ZVJCVOA55NDZJKWIYZ2AZWKA/action/replication_record"}},"created_at":"2026-05-18T00:20:46.834092+00:00","updated_at":"2026-05-18T00:20:46.834092+00:00"}