{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:FP4QPIOCWIN2HRFCRNLCC7MVBF","short_pith_number":"pith:FP4QPIOC","schema_version":"1.0","canonical_sha256":"2bf907a1c2b21ba3c4a28b56217d95095c363024de04dd99dd1e1246c74bf4df","source":{"kind":"arxiv","id":"1606.05870","version":4},"attestation_state":"computed","paper":{"title":"Some Novel Features in 2D Non-Abelian Theory: BRST Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. K. Kureel, N. Srinivas, R. P. Malik, S. Kumar","submitted_at":"2016-06-19T13:40:08Z","abstract_excerpt":"Within the framework of Becchi-Rouet-Stora-Tyutin (BRST) formalism, we discuss some novel features of a two (1+1)-dimensional (2D) non-Abelian 1-form gauge theory (without any interaction with matter fields). Besides the usual off-shell nilpotent and absolutely anticommutating (anti-)BRST symmetry transformations, we discuss the off-shell nilpotent and absolutely anticommutating (anti-)co-BRST symmetry transformations. Particularly, we lay emphasis on the existence of the coupled (but equivalent) Lagrangian densities of the 2D non-Abelian theory in view of the presence of (anti-)co-BRST symmet"},"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":"1606.05870","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-06-19T13:40:08Z","cross_cats_sorted":[],"title_canon_sha256":"03dee7f5db9f10de95794ce8e70293f113a3253c3fdb992ba8aee1a67245d23c","abstract_canon_sha256":"1601c9197a0162b9235f09add9abd98e1e5c91a1d8d4f76450585dc515f6f64d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:24.955672Z","signature_b64":"b06IoaPLf1yUZLKktGPnFSXTdPllbVD0BWqHB1pASl/qC3fEA/WUavDRrkjiN6Vrgt/SOkCOgZRfSuaQlQbjCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bf907a1c2b21ba3c4a28b56217d95095c363024de04dd99dd1e1246c74bf4df","last_reissued_at":"2026-05-18T00:35:24.955069Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:24.955069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Some Novel Features in 2D Non-Abelian Theory: BRST Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. K. Kureel, N. Srinivas, R. P. Malik, S. Kumar","submitted_at":"2016-06-19T13:40:08Z","abstract_excerpt":"Within the framework of Becchi-Rouet-Stora-Tyutin (BRST) formalism, we discuss some novel features of a two (1+1)-dimensional (2D) non-Abelian 1-form gauge theory (without any interaction with matter fields). Besides the usual off-shell nilpotent and absolutely anticommutating (anti-)BRST symmetry transformations, we discuss the off-shell nilpotent and absolutely anticommutating (anti-)co-BRST symmetry transformations. Particularly, we lay emphasis on the existence of the coupled (but equivalent) Lagrangian densities of the 2D non-Abelian theory in view of the presence of (anti-)co-BRST symmet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.05870","kind":"arxiv","version":4},"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":"1606.05870","created_at":"2026-05-18T00:35:24.955182+00:00"},{"alias_kind":"arxiv_version","alias_value":"1606.05870v4","created_at":"2026-05-18T00:35:24.955182+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.05870","created_at":"2026-05-18T00:35:24.955182+00:00"},{"alias_kind":"pith_short_12","alias_value":"FP4QPIOCWIN2","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"FP4QPIOCWIN2HRFC","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"FP4QPIOC","created_at":"2026-05-18T12:30:15.759754+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/FP4QPIOCWIN2HRFCRNLCC7MVBF","json":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF.json","graph_json":"https://pith.science/api/pith-number/FP4QPIOCWIN2HRFCRNLCC7MVBF/graph.json","events_json":"https://pith.science/api/pith-number/FP4QPIOCWIN2HRFCRNLCC7MVBF/events.json","paper":"https://pith.science/paper/FP4QPIOC"},"agent_actions":{"view_html":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF","download_json":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF.json","view_paper":"https://pith.science/paper/FP4QPIOC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1606.05870&json=true","fetch_graph":"https://pith.science/api/pith-number/FP4QPIOCWIN2HRFCRNLCC7MVBF/graph.json","fetch_events":"https://pith.science/api/pith-number/FP4QPIOCWIN2HRFCRNLCC7MVBF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF/action/storage_attestation","attest_author":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF/action/author_attestation","sign_citation":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF/action/citation_signature","submit_replication":"https://pith.science/pith/FP4QPIOCWIN2HRFCRNLCC7MVBF/action/replication_record"}},"created_at":"2026-05-18T00:35:24.955182+00:00","updated_at":"2026-05-18T00:35:24.955182+00:00"}