{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:R22KXMYDDENWGFCAVJGLL57LQU","short_pith_number":"pith:R22KXMYD","schema_version":"1.0","canonical_sha256":"8eb4abb303191b631440aa4cb5f7eb853e8227df9ab1c71c063e20e2ee948dbb","source":{"kind":"arxiv","id":"2106.16205","version":1},"attestation_state":"computed","paper":{"title":"Infrared propagators of Yang-Mills-Chern-Simons theories in linear covariant gauges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Antonio D. Pereira, Diego R. Granado, Igor F. Justo, Luigi C. Ferreira","submitted_at":"2021-06-30T16:58:48Z","abstract_excerpt":"Recent works have explored non-perturbative effects due to the existence of (infinitesimal) Gribov copies in Yang-Mills-Chern-Simons theories in three Euclidean dimensions. In particular, the removal of such copies modify the gauge field propagator by a self-consistent dynamically generated mass parameter, the Gribov parameter. Due to the interplay with the topological mass introduced by the Chern-Simons term, the propagator features a non-trivial set of phases with poles of different nature, leading to the possible interpretation of a confinfing to deconfining phase transition. Inhere, we res"},"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":"2106.16205","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-06-30T16:58:48Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"6466b9b163da4bb59b155d5f50ca730abeb8eccb6cef89a0864b38e7ed4b02d1","abstract_canon_sha256":"0e4b3baae917589d02211a4be75e1cd47ca8ca1d125dcd63c89273802d73b899"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:08:34.929612Z","signature_b64":"0uj/WYIAakkHvQ5grcRG5PJuKfJ9YQ/qP18sQp5Krpw3ac1Zm4VOHclHoG2n9AFXZYS3gmYkAUUxW887LMogAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8eb4abb303191b631440aa4cb5f7eb853e8227df9ab1c71c063e20e2ee948dbb","last_reissued_at":"2026-07-05T03:08:34.929266Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:08:34.929266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Infrared propagators of Yang-Mills-Chern-Simons theories in linear covariant gauges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Antonio D. Pereira, Diego R. Granado, Igor F. Justo, Luigi C. Ferreira","submitted_at":"2021-06-30T16:58:48Z","abstract_excerpt":"Recent works have explored non-perturbative effects due to the existence of (infinitesimal) Gribov copies in Yang-Mills-Chern-Simons theories in three Euclidean dimensions. In particular, the removal of such copies modify the gauge field propagator by a self-consistent dynamically generated mass parameter, the Gribov parameter. Due to the interplay with the topological mass introduced by the Chern-Simons term, the propagator features a non-trivial set of phases with poles of different nature, leading to the possible interpretation of a confinfing to deconfining phase transition. Inhere, we res"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.16205","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.16205/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2106.16205","created_at":"2026-07-05T03:08:34.929319+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.16205v1","created_at":"2026-07-05T03:08:34.929319+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.16205","created_at":"2026-07-05T03:08:34.929319+00:00"},{"alias_kind":"pith_short_12","alias_value":"R22KXMYDDENW","created_at":"2026-07-05T03:08:34.929319+00:00"},{"alias_kind":"pith_short_16","alias_value":"R22KXMYDDENWGFCA","created_at":"2026-07-05T03:08:34.929319+00:00"},{"alias_kind":"pith_short_8","alias_value":"R22KXMYD","created_at":"2026-07-05T03:08:34.929319+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.03284","citing_title":"Finiteness of the Yang-Mills-Chern-Simons action in linear covariant gauges by taking into account gauge copies","ref_index":84,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU","json":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU.json","graph_json":"https://pith.science/api/pith-number/R22KXMYDDENWGFCAVJGLL57LQU/graph.json","events_json":"https://pith.science/api/pith-number/R22KXMYDDENWGFCAVJGLL57LQU/events.json","paper":"https://pith.science/paper/R22KXMYD"},"agent_actions":{"view_html":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU","download_json":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU.json","view_paper":"https://pith.science/paper/R22KXMYD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.16205&json=true","fetch_graph":"https://pith.science/api/pith-number/R22KXMYDDENWGFCAVJGLL57LQU/graph.json","fetch_events":"https://pith.science/api/pith-number/R22KXMYDDENWGFCAVJGLL57LQU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU/action/storage_attestation","attest_author":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU/action/author_attestation","sign_citation":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU/action/citation_signature","submit_replication":"https://pith.science/pith/R22KXMYDDENWGFCAVJGLL57LQU/action/replication_record"}},"created_at":"2026-07-05T03:08:34.929319+00:00","updated_at":"2026-07-05T03:08:34.929319+00:00"}