{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:RKX5FXB5ZZQFIHXO7ZB6J7VSAL","short_pith_number":"pith:RKX5FXB5","canonical_record":{"source":{"id":"1409.1735","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-05T10:55:45Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"15905a966c4e8cb6d3b8bc86070c33164ed73d0b8ccfe59b1ef78b6c3578f15f","abstract_canon_sha256":"71494cd9a7abd9af39426d4c675d0b93e72985aac1e9fb730b636b6d58707ada"},"schema_version":"1.0"},"canonical_sha256":"8aafd2dc3dce60541eeefe43e4feb202d9dcd945550ad0955a993e06235aeea5","source":{"kind":"arxiv","id":"1409.1735","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.1735","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"arxiv_version","alias_value":"1409.1735v3","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.1735","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"pith_short_12","alias_value":"RKX5FXB5ZZQF","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RKX5FXB5ZZQFIHXO","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RKX5FXB5","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:RKX5FXB5ZZQFIHXO7ZB6J7VSAL","target":"record","payload":{"canonical_record":{"source":{"id":"1409.1735","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-05T10:55:45Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"15905a966c4e8cb6d3b8bc86070c33164ed73d0b8ccfe59b1ef78b6c3578f15f","abstract_canon_sha256":"71494cd9a7abd9af39426d4c675d0b93e72985aac1e9fb730b636b6d58707ada"},"schema_version":"1.0"},"canonical_sha256":"8aafd2dc3dce60541eeefe43e4feb202d9dcd945550ad0955a993e06235aeea5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:31.483152Z","signature_b64":"BF6KSUWcDuWYRAHqjs/TEs0JAn2sYhDoo0cjlTu96XcaFX/qNxMngCgj3P97TVa+LYfG6v8sSBcVe1LTltZVAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8aafd2dc3dce60541eeefe43e4feb202d9dcd945550ad0955a993e06235aeea5","last_reissued_at":"2026-05-18T02:18:31.482497Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:31.482497Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.1735","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:18:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OZseY5fve9oLSjYpdGcXEuFOKmoNV7VyI/vsP13MDdkmlU3G3TQp+0Fw8R9OPh6CZ6wlq0U5RXEoVpoWRMcdAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:39:37.722126Z"},"content_sha256":"a7a25acd81b766c5294e6eeef88a124deafeb69ee0c974dec4d2d5034e60834e","schema_version":"1.0","event_id":"sha256:a7a25acd81b766c5294e6eeef88a124deafeb69ee0c974dec4d2d5034e60834e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:RKX5FXB5ZZQFIHXO7ZB6J7VSAL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Generalized BRST symmetry for arbitrary spin conformal field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Bhabani Prasad Mandal, Sudhaker Upadhyay","submitted_at":"2014-09-05T10:55:45Z","abstract_excerpt":"We develop the finite field-dependent BRST (FFBRST) transformation for arbitrary spin-s conformal field theories. We discuss the novel features of the FFBRST transformation in these systems. To illustrate the results we consider the spin-1 and spin-2 conformal field theories in two examples. Within the formalism we found that FFBRST transformation connects the generating functionals of spin-1 and spin-2 conformal field theories in linear and non-linear gauges. Further, the conformal field theories in the framework of FFBRST transformation are also analysed in Batalin-Vilkovisky (BV) formulatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.1735","kind":"arxiv","version":3},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:18:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E053h2Ot48sjO0D1LgPx2+/DlExz2V0uHY1TRWY9P7VjX/RBI1WZYF95gZbBobUnHccP3JI8QcjkvQ6IefLBCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:39:37.722489Z"},"content_sha256":"2836a05e0923382ed97c59be9fde3c0a1bd7a75cefb7f603b91ed1fb2629bf59","schema_version":"1.0","event_id":"sha256:2836a05e0923382ed97c59be9fde3c0a1bd7a75cefb7f603b91ed1fb2629bf59"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/bundle.json","state_url":"https://pith.science/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-31T03:39:37Z","links":{"resolver":"https://pith.science/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL","bundle":"https://pith.science/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/bundle.json","state":"https://pith.science/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RKX5FXB5ZZQFIHXO7ZB6J7VSAL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:RKX5FXB5ZZQFIHXO7ZB6J7VSAL","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"71494cd9a7abd9af39426d4c675d0b93e72985aac1e9fb730b636b6d58707ada","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-05T10:55:45Z","title_canon_sha256":"15905a966c4e8cb6d3b8bc86070c33164ed73d0b8ccfe59b1ef78b6c3578f15f"},"schema_version":"1.0","source":{"id":"1409.1735","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.1735","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"arxiv_version","alias_value":"1409.1735v3","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.1735","created_at":"2026-05-18T02:18:31Z"},{"alias_kind":"pith_short_12","alias_value":"RKX5FXB5ZZQF","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RKX5FXB5ZZQFIHXO","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RKX5FXB5","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:2836a05e0923382ed97c59be9fde3c0a1bd7a75cefb7f603b91ed1fb2629bf59","target":"graph","created_at":"2026-05-18T02:18:31Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We develop the finite field-dependent BRST (FFBRST) transformation for arbitrary spin-s conformal field theories. We discuss the novel features of the FFBRST transformation in these systems. To illustrate the results we consider the spin-1 and spin-2 conformal field theories in two examples. Within the formalism we found that FFBRST transformation connects the generating functionals of spin-1 and spin-2 conformal field theories in linear and non-linear gauges. Further, the conformal field theories in the framework of FFBRST transformation are also analysed in Batalin-Vilkovisky (BV) formulatio","authors_text":"Bhabani Prasad Mandal, Sudhaker Upadhyay","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-05T10:55:45Z","title":"Generalized BRST symmetry for arbitrary spin conformal field theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.1735","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a7a25acd81b766c5294e6eeef88a124deafeb69ee0c974dec4d2d5034e60834e","target":"record","created_at":"2026-05-18T02:18:31Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"71494cd9a7abd9af39426d4c675d0b93e72985aac1e9fb730b636b6d58707ada","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-05T10:55:45Z","title_canon_sha256":"15905a966c4e8cb6d3b8bc86070c33164ed73d0b8ccfe59b1ef78b6c3578f15f"},"schema_version":"1.0","source":{"id":"1409.1735","kind":"arxiv","version":3}},"canonical_sha256":"8aafd2dc3dce60541eeefe43e4feb202d9dcd945550ad0955a993e06235aeea5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8aafd2dc3dce60541eeefe43e4feb202d9dcd945550ad0955a993e06235aeea5","first_computed_at":"2026-05-18T02:18:31.482497Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:18:31.482497Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BF6KSUWcDuWYRAHqjs/TEs0JAn2sYhDoo0cjlTu96XcaFX/qNxMngCgj3P97TVa+LYfG6v8sSBcVe1LTltZVAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:18:31.483152Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.1735","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a7a25acd81b766c5294e6eeef88a124deafeb69ee0c974dec4d2d5034e60834e","sha256:2836a05e0923382ed97c59be9fde3c0a1bd7a75cefb7f603b91ed1fb2629bf59"],"state_sha256":"ea6e553fb50a0d8716857fead83602d1787f7db1cf55518516ea126cec676c56"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Kqfm4WiaZ0ZnSvR1SAUP+RYov93w3ambN8Qj+GtqrgmdYaehDub7sI0DTvAgTMAjZ2VyobRpL3lw0eNi0GL+Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T03:39:37.724621Z","bundle_sha256":"4874183a00e73422d1e8d74c58b36daf343ff694b788a3dd535ec0a4f8535ac2"}}