{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:Q4IA6TCQ35DXIXOBTTXPTR4VUO","short_pith_number":"pith:Q4IA6TCQ","schema_version":"1.0","canonical_sha256":"87100f4c50df47745dc19ceef9c795a39dce6a7a64607c6614e56f4fabec85b4","source":{"kind":"arxiv","id":"2605.16172","version":1},"attestation_state":"computed","paper":{"title":"Background-Equivariant BRST Observables and i-Particle Propagators from an Auxiliary Quartet in SU(3) Yang-Mills","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M. M. Amaral, V.E.R.Lemes","submitted_at":"2026-05-15T16:51:08Z","abstract_excerpt":"In this work, we construct a BRST-exact quartet mechanism in $SU(3)$ Yang-Mills theory in the Landau gauge. The quartet sector is cohomologically trivial in the standard vacuum, ensuring equivalence to pure Yang-Mills theory. The transformation rules carry both commutator and anticommutator structures, enlarging the field content from eight to nine degrees of freedom.\n  Working in a prescribed Cartan-oriented background (compatible with the classical equations of motion), the theory induces a mass matrix reproducing the distinct $i$-particle propagator structure of earlier replica models witho"},"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":"2605.16172","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-05-15T16:51:08Z","cross_cats_sorted":[],"title_canon_sha256":"5cd343be6f2709c9f057ec77868caba45ce1bb6ede42464cd73edd9025bf2968","abstract_canon_sha256":"d52d73ce12d640030c304c1636b8cb4ae96d4b61677604a89cc4c4a5bf857cea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:01:56.065728Z","signature_b64":"6mkiDy1LIoyGez8CCHOoSMLxddB4boLR2Zug+g6XVw8SXg1zAdzyeqjIlgMF8N3KIoFXWTWMCjFLsWLtrfmlDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"87100f4c50df47745dc19ceef9c795a39dce6a7a64607c6614e56f4fabec85b4","last_reissued_at":"2026-05-20T00:01:56.064955Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:01:56.064955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Background-Equivariant BRST Observables and i-Particle Propagators from an Auxiliary Quartet in SU(3) Yang-Mills","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M. M. Amaral, V.E.R.Lemes","submitted_at":"2026-05-15T16:51:08Z","abstract_excerpt":"In this work, we construct a BRST-exact quartet mechanism in $SU(3)$ Yang-Mills theory in the Landau gauge. The quartet sector is cohomologically trivial in the standard vacuum, ensuring equivalence to pure Yang-Mills theory. The transformation rules carry both commutator and anticommutator structures, enlarging the field content from eight to nine degrees of freedom.\n  Working in a prescribed Cartan-oriented background (compatible with the classical equations of motion), the theory induces a mass matrix reproducing the distinct $i$-particle propagator structure of earlier replica models witho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.16172","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/2605.16172/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"cited_work_retraction","ran_at":"2026-05-19T17:52:14.587273Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T17:33:31.028892Z","status":"skipped","version":"1.0.0","findings_count":0},{"name":"external_links","ran_at":"2026-05-19T17:31:45.582527Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T16:41:55.427465Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"ecf1c7f182279ab00b73a38d265dc1935e393b77ef300a451cebb4541601ffd4"},"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":"2605.16172","created_at":"2026-05-20T00:01:56.065089+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.16172v1","created_at":"2026-05-20T00:01:56.065089+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.16172","created_at":"2026-05-20T00:01:56.065089+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q4IA6TCQ35DX","created_at":"2026-05-20T00:01:56.065089+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q4IA6TCQ35DXIXOB","created_at":"2026-05-20T00:01:56.065089+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q4IA6TCQ","created_at":"2026-05-20T00:01:56.065089+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/Q4IA6TCQ35DXIXOBTTXPTR4VUO","json":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO.json","graph_json":"https://pith.science/api/pith-number/Q4IA6TCQ35DXIXOBTTXPTR4VUO/graph.json","events_json":"https://pith.science/api/pith-number/Q4IA6TCQ35DXIXOBTTXPTR4VUO/events.json","paper":"https://pith.science/paper/Q4IA6TCQ"},"agent_actions":{"view_html":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO","download_json":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO.json","view_paper":"https://pith.science/paper/Q4IA6TCQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.16172&json=true","fetch_graph":"https://pith.science/api/pith-number/Q4IA6TCQ35DXIXOBTTXPTR4VUO/graph.json","fetch_events":"https://pith.science/api/pith-number/Q4IA6TCQ35DXIXOBTTXPTR4VUO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO/action/storage_attestation","attest_author":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO/action/author_attestation","sign_citation":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO/action/citation_signature","submit_replication":"https://pith.science/pith/Q4IA6TCQ35DXIXOBTTXPTR4VUO/action/replication_record"}},"created_at":"2026-05-20T00:01:56.065089+00:00","updated_at":"2026-05-20T00:01:56.065089+00:00"}