{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:SZKZF2X2I4IC3BMKHXYYOYUC74","short_pith_number":"pith:SZKZF2X2","schema_version":"1.0","canonical_sha256":"965592eafa47102d858a3df1876282ff1cff198fff89dc829d71ef9574bda45b","source":{"kind":"arxiv","id":"hep-th/0508226","version":5},"attestation_state":"computed","paper":{"title":"Augmented Superfield Approach To Unique Nilpotent Symmetries For Complex Scalar Fields In QED","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"BHU), Phys. Deptt., R. P. Malik (Bose National Centre & CAS","submitted_at":"2005-08-30T15:50:33Z","abstract_excerpt":"The derivation of the exact and unique nilpotent Becchi-Rouet-Stora-Tyutin (BRST)- and anti-BRST symmetries for the matter fields, present in any arbitrary interacting gauge theory, has been a long-standing problem in the framework of superfield approach to BRST formalism. These nilpotent symmetry transformations are deduced for the four (3 + 1)-dimensional (4D) complex scalar fields, coupled to the U(1) gauge field, in the framework of augmented superfield formalism. This interacting gauge theory (i.e. QED) is considered on a six (4, 2)-dimensional supermanifold parametrized by four even spac"},"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":"hep-th/0508226","kind":"arxiv","version":5},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-08-30T15:50:33Z","cross_cats_sorted":[],"title_canon_sha256":"ad9e3829c7bcfa079c116e24b3e39f34e6fc5d8989a25cd41d7b40f2988ca2c4","abstract_canon_sha256":"098baf8e1e2131e735a93489ec57f0367eaddb9915dddf5e73915e4e4865ae3b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:54.743672Z","signature_b64":"hZukE+H3ikaiIIkBuBAdqN/iQcTrXcKdhdx3EHXJZDVi5SiCSuQd31hN+nl7JLvuPbCjEiFuzmNPv8vgOsSPDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"965592eafa47102d858a3df1876282ff1cff198fff89dc829d71ef9574bda45b","last_reissued_at":"2026-05-18T04:17:54.743068Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:54.743068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Augmented Superfield Approach To Unique Nilpotent Symmetries For Complex Scalar Fields In QED","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"BHU), Phys. Deptt., R. P. Malik (Bose National Centre & CAS","submitted_at":"2005-08-30T15:50:33Z","abstract_excerpt":"The derivation of the exact and unique nilpotent Becchi-Rouet-Stora-Tyutin (BRST)- and anti-BRST symmetries for the matter fields, present in any arbitrary interacting gauge theory, has been a long-standing problem in the framework of superfield approach to BRST formalism. These nilpotent symmetry transformations are deduced for the four (3 + 1)-dimensional (4D) complex scalar fields, coupled to the U(1) gauge field, in the framework of augmented superfield formalism. This interacting gauge theory (i.e. QED) is considered on a six (4, 2)-dimensional supermanifold parametrized by four even spac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0508226","kind":"arxiv","version":5},"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":"hep-th/0508226","created_at":"2026-05-18T04:17:54.743158+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0508226v5","created_at":"2026-05-18T04:17:54.743158+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0508226","created_at":"2026-05-18T04:17:54.743158+00:00"},{"alias_kind":"pith_short_12","alias_value":"SZKZF2X2I4IC","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"SZKZF2X2I4IC3BMK","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"SZKZF2X2","created_at":"2026-05-18T12:25:53.335082+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/SZKZF2X2I4IC3BMKHXYYOYUC74","json":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74.json","graph_json":"https://pith.science/api/pith-number/SZKZF2X2I4IC3BMKHXYYOYUC74/graph.json","events_json":"https://pith.science/api/pith-number/SZKZF2X2I4IC3BMKHXYYOYUC74/events.json","paper":"https://pith.science/paper/SZKZF2X2"},"agent_actions":{"view_html":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74","download_json":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74.json","view_paper":"https://pith.science/paper/SZKZF2X2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0508226&json=true","fetch_graph":"https://pith.science/api/pith-number/SZKZF2X2I4IC3BMKHXYYOYUC74/graph.json","fetch_events":"https://pith.science/api/pith-number/SZKZF2X2I4IC3BMKHXYYOYUC74/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74/action/storage_attestation","attest_author":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74/action/author_attestation","sign_citation":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74/action/citation_signature","submit_replication":"https://pith.science/pith/SZKZF2X2I4IC3BMKHXYYOYUC74/action/replication_record"}},"created_at":"2026-05-18T04:17:54.743158+00:00","updated_at":"2026-05-18T04:17:54.743158+00:00"}