{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:UX5VNOWCPEVXY4AXGPNIZMTHGS","short_pith_number":"pith:UX5VNOWC","canonical_record":{"source":{"id":"1009.5859","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-29T12:19:31Z","cross_cats_sorted":[],"title_canon_sha256":"ba6347860e5413bc2718760f58bacbefd7deea35681e656979b02e7689b32a70","abstract_canon_sha256":"3a6fcc0ce76525cc77bb4feae42aeee5460cc312e1cb555ec234cfaa388695b9"},"schema_version":"1.0"},"canonical_sha256":"a5fb56bac2792b7c701733da8cb26734a70f6d170422f85ecc84165f5cad8ec7","source":{"kind":"arxiv","id":"1009.5859","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.5859","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"arxiv_version","alias_value":"1009.5859v1","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.5859","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"pith_short_12","alias_value":"UX5VNOWCPEVX","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"UX5VNOWCPEVXY4AX","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"UX5VNOWC","created_at":"2026-05-18T12:26:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:UX5VNOWCPEVXY4AXGPNIZMTHGS","target":"record","payload":{"canonical_record":{"source":{"id":"1009.5859","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-29T12:19:31Z","cross_cats_sorted":[],"title_canon_sha256":"ba6347860e5413bc2718760f58bacbefd7deea35681e656979b02e7689b32a70","abstract_canon_sha256":"3a6fcc0ce76525cc77bb4feae42aeee5460cc312e1cb555ec234cfaa388695b9"},"schema_version":"1.0"},"canonical_sha256":"a5fb56bac2792b7c701733da8cb26734a70f6d170422f85ecc84165f5cad8ec7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:38.719569Z","signature_b64":"t52byMS7n5PhwNkBk/ToLYv6eTQWK00G5KweCg+vwbPoDNnK0NxmaYsWRVbXiOo8eTmSXDBczC5N39eWvEihAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5fb56bac2792b7c701733da8cb26734a70f6d170422f85ecc84165f5cad8ec7","last_reissued_at":"2026-05-18T04:33:38.719058Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:38.719058Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1009.5859","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:33:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Pcu9rflEfWPoUS0IqXRpdVM8Tqx9h0RKQhVlrta1o3M2wgC9F0CSi2b6t1/CpeyquabKsQUEWzC6GTHFcIIdBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T21:31:25.287736Z"},"content_sha256":"e38345e130f0f0fd90df9788b61d05e243e0031d6f99d0817567b7b2984f2184","schema_version":"1.0","event_id":"sha256:e38345e130f0f0fd90df9788b61d05e243e0031d6f99d0817567b7b2984f2184"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:UX5VNOWCPEVXY4AXGPNIZMTHGS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite nilpotent symmetry in Batalin-Vilkovisky formalism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bhabani Prasad Mandal, Sudhaker Upadhyay, Sumit Kumar Rai","submitted_at":"2010-09-29T12:19:31Z","abstract_excerpt":"We consider the Batalin-Vilkovisky formulation of both 1-form and 2-form gauge theories, in the context of generalized BRST transformations with finite field dependent parameter. In the usual Faddeev-Popov formulation of gauge theories such finite field dependent BRST (FFBRST) transformations do not leave the generating functionals invariant as the path integral measure changes in a non-trivial way for a finite transformations. Here we show that FFBRST transformation, with appropriate choice of finite field-dependent parameter, is symmetry of the generating functionals in the Batalin-Vilkovisk"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.5859","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":""},"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":"2026-05-18T04:33:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Yi932llq0ilpplW5ypF+SwXfkNJdcLzm74wxvmPkpk0AmkAP4XyRm3lKugTX13At9rxEX3WUAkT7rMTr9oUkCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T21:31:25.288513Z"},"content_sha256":"7e1c1d7b6d2b907a4958c068e40cf3cf889b906d36a47ca0018c66a6ad8a63a2","schema_version":"1.0","event_id":"sha256:7e1c1d7b6d2b907a4958c068e40cf3cf889b906d36a47ca0018c66a6ad8a63a2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/bundle.json","state_url":"https://pith.science/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/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":"2026-05-30T21:31:25Z","links":{"resolver":"https://pith.science/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS","bundle":"https://pith.science/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/bundle.json","state":"https://pith.science/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UX5VNOWCPEVXY4AXGPNIZMTHGS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:UX5VNOWCPEVXY4AXGPNIZMTHGS","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":"3a6fcc0ce76525cc77bb4feae42aeee5460cc312e1cb555ec234cfaa388695b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-29T12:19:31Z","title_canon_sha256":"ba6347860e5413bc2718760f58bacbefd7deea35681e656979b02e7689b32a70"},"schema_version":"1.0","source":{"id":"1009.5859","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.5859","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"arxiv_version","alias_value":"1009.5859v1","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.5859","created_at":"2026-05-18T04:33:38Z"},{"alias_kind":"pith_short_12","alias_value":"UX5VNOWCPEVX","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"UX5VNOWCPEVXY4AX","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"UX5VNOWC","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:7e1c1d7b6d2b907a4958c068e40cf3cf889b906d36a47ca0018c66a6ad8a63a2","target":"graph","created_at":"2026-05-18T04:33:38Z","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 consider the Batalin-Vilkovisky formulation of both 1-form and 2-form gauge theories, in the context of generalized BRST transformations with finite field dependent parameter. In the usual Faddeev-Popov formulation of gauge theories such finite field dependent BRST (FFBRST) transformations do not leave the generating functionals invariant as the path integral measure changes in a non-trivial way for a finite transformations. Here we show that FFBRST transformation, with appropriate choice of finite field-dependent parameter, is symmetry of the generating functionals in the Batalin-Vilkovisk","authors_text":"Bhabani Prasad Mandal, Sudhaker Upadhyay, Sumit Kumar Rai","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-29T12:19:31Z","title":"Finite nilpotent symmetry in Batalin-Vilkovisky formalism"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.5859","kind":"arxiv","version":1},"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:e38345e130f0f0fd90df9788b61d05e243e0031d6f99d0817567b7b2984f2184","target":"record","created_at":"2026-05-18T04:33:38Z","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":"3a6fcc0ce76525cc77bb4feae42aeee5460cc312e1cb555ec234cfaa388695b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-29T12:19:31Z","title_canon_sha256":"ba6347860e5413bc2718760f58bacbefd7deea35681e656979b02e7689b32a70"},"schema_version":"1.0","source":{"id":"1009.5859","kind":"arxiv","version":1}},"canonical_sha256":"a5fb56bac2792b7c701733da8cb26734a70f6d170422f85ecc84165f5cad8ec7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a5fb56bac2792b7c701733da8cb26734a70f6d170422f85ecc84165f5cad8ec7","first_computed_at":"2026-05-18T04:33:38.719058Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:33:38.719058Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"t52byMS7n5PhwNkBk/ToLYv6eTQWK00G5KweCg+vwbPoDNnK0NxmaYsWRVbXiOo8eTmSXDBczC5N39eWvEihAg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:33:38.719569Z","signed_message":"canonical_sha256_bytes"},"source_id":"1009.5859","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e38345e130f0f0fd90df9788b61d05e243e0031d6f99d0817567b7b2984f2184","sha256:7e1c1d7b6d2b907a4958c068e40cf3cf889b906d36a47ca0018c66a6ad8a63a2"],"state_sha256":"140b3f75fd5e1d51bf789f6183f3b8336dc041f209fbade4d63ea4453d6e2754"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"owiIfog799c7QJHXgU8wAI8yegX3ZbcLdO/OWbcmNwHO1jmjRQZ6230lot97VPHOQ7/ZpSS+HAkdVJeL4Rr1CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T21:31:25.292226Z","bundle_sha256":"5f4fe4a8d8449b2d74ec9739c85defec562b0fd9523077517f4a04fdcca027e1"}}