{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:AQDQ7DELI5UOOCFFI6RQFR4UVD","short_pith_number":"pith:AQDQ7DEL","schema_version":"1.0","canonical_sha256":"04070f8c8b4768e708a547a302c794a8e4c951875a0b4b6466200dc4f6a3f502","source":{"kind":"arxiv","id":"1311.5707","version":1},"attestation_state":"computed","paper":{"title":"Coulomb gauge on the lattice: From zero to finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Giuseppe Burgio, Hannes Vogt, Hugo Reinhardt, Markus Quandt","submitted_at":"2013-11-22T10:45:36Z","abstract_excerpt":"Our previous studies of Coulomb gauge Yang-Mills theory are extended to finite temperature. We investigate the SU(2) static gluon and ghost propagators and show results for the Coulomb potential, with a focus on the Gribov ambiguity. To compute these quantities at high temperatures and to solve scaling violations we use the anisotropic Wilson gauge action."},"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":"1311.5707","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-11-22T10:45:36Z","cross_cats_sorted":[],"title_canon_sha256":"fa69456b2bc7f635cca78afa64ae5489a6dc65062197267ac6fd503576e4489f","abstract_canon_sha256":"75ecce279040566841428f083d91a3508a86e56ded8778b0dde21e14b426ff6e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:23.473164Z","signature_b64":"Q1uYcyV0XmE6bPWbuLXtjHTLyrT/3Uu/N9KXDXVqHAYYlaWp9LJseBCEERNq/eYu0BQ2uQUTE6Gz84wFnV/PCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04070f8c8b4768e708a547a302c794a8e4c951875a0b4b6466200dc4f6a3f502","last_reissued_at":"2026-05-18T03:06:23.472477Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:23.472477Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coulomb gauge on the lattice: From zero to finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Giuseppe Burgio, Hannes Vogt, Hugo Reinhardt, Markus Quandt","submitted_at":"2013-11-22T10:45:36Z","abstract_excerpt":"Our previous studies of Coulomb gauge Yang-Mills theory are extended to finite temperature. We investigate the SU(2) static gluon and ghost propagators and show results for the Coulomb potential, with a focus on the Gribov ambiguity. To compute these quantities at high temperatures and to solve scaling violations we use the anisotropic Wilson gauge action."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.5707","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":"1311.5707","created_at":"2026-05-18T03:06:23.472583+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.5707v1","created_at":"2026-05-18T03:06:23.472583+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.5707","created_at":"2026-05-18T03:06:23.472583+00:00"},{"alias_kind":"pith_short_12","alias_value":"AQDQ7DELI5UO","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"AQDQ7DELI5UOOCFF","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"AQDQ7DEL","created_at":"2026-05-18T12:27:38.830355+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/AQDQ7DELI5UOOCFFI6RQFR4UVD","json":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD.json","graph_json":"https://pith.science/api/pith-number/AQDQ7DELI5UOOCFFI6RQFR4UVD/graph.json","events_json":"https://pith.science/api/pith-number/AQDQ7DELI5UOOCFFI6RQFR4UVD/events.json","paper":"https://pith.science/paper/AQDQ7DEL"},"agent_actions":{"view_html":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD","download_json":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD.json","view_paper":"https://pith.science/paper/AQDQ7DEL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.5707&json=true","fetch_graph":"https://pith.science/api/pith-number/AQDQ7DELI5UOOCFFI6RQFR4UVD/graph.json","fetch_events":"https://pith.science/api/pith-number/AQDQ7DELI5UOOCFFI6RQFR4UVD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD/action/storage_attestation","attest_author":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD/action/author_attestation","sign_citation":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD/action/citation_signature","submit_replication":"https://pith.science/pith/AQDQ7DELI5UOOCFFI6RQFR4UVD/action/replication_record"}},"created_at":"2026-05-18T03:06:23.472583+00:00","updated_at":"2026-05-18T03:06:23.472583+00:00"}