{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:2R5S7EVXXEUQDMEZMQOEG6OT7Y","short_pith_number":"pith:2R5S7EVX","canonical_record":{"source":{"id":"1112.6303","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-29T13:26:32Z","cross_cats_sorted":[],"title_canon_sha256":"4e58823651d47618f44d7bc3513106f2488b556c4a3730355c3ceb2ce800452d","abstract_canon_sha256":"5d54f9597ca317c8951c1d7323c3796475387c5fb953dda33c48648cc43f2746"},"schema_version":"1.0"},"canonical_sha256":"d47b2f92b7b92901b099641c4379d3fe28a4ed17fbb78f2563bf6284ba9ac255","source":{"kind":"arxiv","id":"1112.6303","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.6303","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"1112.6303v2","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.6303","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"2R5S7EVXXEUQ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"2R5S7EVXXEUQDMEZ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"2R5S7EVX","created_at":"2026-05-18T12:26:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:2R5S7EVXXEUQDMEZMQOEG6OT7Y","target":"record","payload":{"canonical_record":{"source":{"id":"1112.6303","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-29T13:26:32Z","cross_cats_sorted":[],"title_canon_sha256":"4e58823651d47618f44d7bc3513106f2488b556c4a3730355c3ceb2ce800452d","abstract_canon_sha256":"5d54f9597ca317c8951c1d7323c3796475387c5fb953dda33c48648cc43f2746"},"schema_version":"1.0"},"canonical_sha256":"d47b2f92b7b92901b099641c4379d3fe28a4ed17fbb78f2563bf6284ba9ac255","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:59.806935Z","signature_b64":"qEkuWttB85DngFCEtHOljGGM8taz49g1OdMRyikHq+pGAegoETfE6FplihjG8mlx7mQrhaL4XTXq4EljDAb9Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d47b2f92b7b92901b099641c4379d3fe28a4ed17fbb78f2563bf6284ba9ac255","last_reissued_at":"2026-05-18T01:58:59.806414Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:59.806414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.6303","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:58:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dPwdH6ATlzjudYNrtjVl16csiXKbcLY0yD68C/AwFf2E6K5bPwnCIgthFwXleLq1h9637motsj8JZjHYTnH9Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:39:47.698891Z"},"content_sha256":"b49d50e76b912fc53d24082fe8547e54ccb4dc0faca8258879ad8885655d674b","schema_version":"1.0","event_id":"sha256:b49d50e76b912fc53d24082fe8547e54ccb4dc0faca8258879ad8885655d674b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:2R5S7EVXXEUQDMEZMQOEG6OT7Y","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Abelian 3-form gauge theory: superfield approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R. P. Malik","submitted_at":"2011-12-29T13:26:32Z","abstract_excerpt":"We discuss a D-dimensional Abelian 3-form gauge theory within the framework of Bonora-Tonin's superfield formalism and derive the off-shell nilpotent and absolutely anticommuting Becchi-Rouet-Stora-Tyutin (BRST) and anti-BRST symmetry transformations for this theory. To pay our homage to Victor I. Ogievetsky (1928-1996), who was one of the inventors of Abelian 2-form (antisymmetric tensor) gauge field, we go a step further and discuss the above D-dimensional Abelian 3-form gauge theory within the framework of BRST formalism and establish that the existence of the (anti-)BRST invariant Curci-Fe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.6303","kind":"arxiv","version":2},"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":"2026-05-18T01:58:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IhVWtM6VqB/9nupVKWNmn2+beQ4t4z9hkggJz6Tor+iNkNUcSVPpX7sfn1i+ndcMJI7enJmFX+imtz6axXczDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:39:47.699969Z"},"content_sha256":"e34ab9979398b330a2d22bb486180462fb3242e01a4b91b003c0522b142c6ea4","schema_version":"1.0","event_id":"sha256:e34ab9979398b330a2d22bb486180462fb3242e01a4b91b003c0522b142c6ea4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/bundle.json","state_url":"https://pith.science/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/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":"2026-08-12T15:39:47Z","links":{"resolver":"https://pith.science/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y","bundle":"https://pith.science/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/bundle.json","state":"https://pith.science/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2R5S7EVXXEUQDMEZMQOEG6OT7Y/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:2R5S7EVXXEUQDMEZMQOEG6OT7Y","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":"5d54f9597ca317c8951c1d7323c3796475387c5fb953dda33c48648cc43f2746","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-29T13:26:32Z","title_canon_sha256":"4e58823651d47618f44d7bc3513106f2488b556c4a3730355c3ceb2ce800452d"},"schema_version":"1.0","source":{"id":"1112.6303","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.6303","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"1112.6303v2","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.6303","created_at":"2026-05-18T01:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"2R5S7EVXXEUQ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"2R5S7EVXXEUQDMEZ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"2R5S7EVX","created_at":"2026-05-18T12:26:18Z"}],"graph_snapshots":[{"event_id":"sha256:e34ab9979398b330a2d22bb486180462fb3242e01a4b91b003c0522b142c6ea4","target":"graph","created_at":"2026-05-18T01:58:59Z","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 discuss a D-dimensional Abelian 3-form gauge theory within the framework of Bonora-Tonin's superfield formalism and derive the off-shell nilpotent and absolutely anticommuting Becchi-Rouet-Stora-Tyutin (BRST) and anti-BRST symmetry transformations for this theory. To pay our homage to Victor I. Ogievetsky (1928-1996), who was one of the inventors of Abelian 2-form (antisymmetric tensor) gauge field, we go a step further and discuss the above D-dimensional Abelian 3-form gauge theory within the framework of BRST formalism and establish that the existence of the (anti-)BRST invariant Curci-Fe","authors_text":"R. P. Malik","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-29T13:26:32Z","title":"Abelian 3-form gauge theory: superfield approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.6303","kind":"arxiv","version":2},"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:b49d50e76b912fc53d24082fe8547e54ccb4dc0faca8258879ad8885655d674b","target":"record","created_at":"2026-05-18T01:58:59Z","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":"5d54f9597ca317c8951c1d7323c3796475387c5fb953dda33c48648cc43f2746","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-29T13:26:32Z","title_canon_sha256":"4e58823651d47618f44d7bc3513106f2488b556c4a3730355c3ceb2ce800452d"},"schema_version":"1.0","source":{"id":"1112.6303","kind":"arxiv","version":2}},"canonical_sha256":"d47b2f92b7b92901b099641c4379d3fe28a4ed17fbb78f2563bf6284ba9ac255","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d47b2f92b7b92901b099641c4379d3fe28a4ed17fbb78f2563bf6284ba9ac255","first_computed_at":"2026-05-18T01:58:59.806414Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:59.806414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qEkuWttB85DngFCEtHOljGGM8taz49g1OdMRyikHq+pGAegoETfE6FplihjG8mlx7mQrhaL4XTXq4EljDAb9Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:59.806935Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.6303","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b49d50e76b912fc53d24082fe8547e54ccb4dc0faca8258879ad8885655d674b","sha256:e34ab9979398b330a2d22bb486180462fb3242e01a4b91b003c0522b142c6ea4"],"state_sha256":"28f6f7d2642ff967430f501811324f5e501421eae0f4ebc14cc00c517f27b3ed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"o2VKFN7WbTV6Jvf2sCFqFcNWVMFOx0wdgK8ay30r76hWKuaL9msfRhPqaxdPSlF1ikOnnxX3c0UsqA6DHjj1AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T15:39:47.729886Z","bundle_sha256":"4e20a6b57c8f4bc485058ec4193c84f5274d5fc0da77bcf266cf239f02b305dd"}}