{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:VSTPDRK26QU5AA72KCPIHNHT7M","short_pith_number":"pith:VSTPDRK2","canonical_record":{"source":{"id":"1710.05336","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-15T13:56:33Z","cross_cats_sorted":[],"title_canon_sha256":"5622eb998429d30e41e5b68815edbb33ee28ac4a928eddae4d0edf2a6d9159aa","abstract_canon_sha256":"2f5a70ae7b3fba92e9f526392dd3d1468c0359fbe9e87aadb6ac27a05fcf4573"},"schema_version":"1.0"},"canonical_sha256":"aca6f1c55af429d003fa509e83b4f3fb079a541b92ecddfa1709e5e08d21c626","source":{"kind":"arxiv","id":"1710.05336","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.05336","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"arxiv_version","alias_value":"1710.05336v4","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.05336","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"pith_short_12","alias_value":"VSTPDRK26QU5","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VSTPDRK26QU5AA72","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VSTPDRK2","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:VSTPDRK26QU5AA72KCPIHNHT7M","target":"record","payload":{"canonical_record":{"source":{"id":"1710.05336","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-15T13:56:33Z","cross_cats_sorted":[],"title_canon_sha256":"5622eb998429d30e41e5b68815edbb33ee28ac4a928eddae4d0edf2a6d9159aa","abstract_canon_sha256":"2f5a70ae7b3fba92e9f526392dd3d1468c0359fbe9e87aadb6ac27a05fcf4573"},"schema_version":"1.0"},"canonical_sha256":"aca6f1c55af429d003fa509e83b4f3fb079a541b92ecddfa1709e5e08d21c626","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:59.551025Z","signature_b64":"gtFymS2C73mltTtBI+19pQZ4pUA0EGn0/XoffLv2BZcR9mkvYGgzjepfnwxB74tTHymn89SEWXgioCBUCn0VCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aca6f1c55af429d003fa509e83b4f3fb079a541b92ecddfa1709e5e08d21c626","last_reissued_at":"2026-05-18T00:24:59.550574Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:59.550574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.05336","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:24:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aUqVRyKicWWnJFipfB9e5XeHnQzKLRdzIW8QcqgOFVbK5fJH50LY3/ENM5XLu8uwi/YvEusJ4kodXL0FM1caBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T05:01:14.779305Z"},"content_sha256":"2eb774413da0c271b4034436ae100a34e99521ca669c869878c861f4ed5b6337","schema_version":"1.0","event_id":"sha256:2eb774413da0c271b4034436ae100a34e99521ca669c869878c861f4ed5b6337"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:VSTPDRK26QU5AA72KCPIHNHT7M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"(Anti-)Chiral Superfield Approach to Interacting Abelian 1-Form Gauge Theories: Nilpotent and Absolutely Anticommuting Charges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Chauhan, R. P. Malik, S. Kumar","submitted_at":"2017-10-15T13:56:33Z","abstract_excerpt":"We derive the off-shell nilpotent (fermionic) (anti-)BRST symmetry transformations by exploiting the (anti-)chiral superfield approach (ACSA) to Becchi-Rouet-Stora-Tyutin (BRST) formalism for the interacting Abelian 1-form gauge theories where there is a coupling between the U(1) Abelian 1-form gauge field and Dirac as well as complex scalar fields. We exploit the (anti-)BRST invariant restrictions on the (anti-)chiral superfields to derive the fermionic symmetries of our present D-dimensional Abelian 1-form gauge theories. The novel observation of our present investigation is the derivation o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.05336","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:24:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l5v5ZR21eVlYrIZG69HKbJ0qCXNgyTcjDR8TfjMLyE4FmqFYeTLhfn7/mLJI20TXpEFiFcusCxAeMRZRgD6RDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T05:01:14.779672Z"},"content_sha256":"0ef6defc6414c0d71da6b05c38412c0ed1d66c0f42ee6f939b70dc953752a748","schema_version":"1.0","event_id":"sha256:0ef6defc6414c0d71da6b05c38412c0ed1d66c0f42ee6f939b70dc953752a748"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VSTPDRK26QU5AA72KCPIHNHT7M/bundle.json","state_url":"https://pith.science/pith/VSTPDRK26QU5AA72KCPIHNHT7M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VSTPDRK26QU5AA72KCPIHNHT7M/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":"2026-07-09T05:01:14Z","links":{"resolver":"https://pith.science/pith/VSTPDRK26QU5AA72KCPIHNHT7M","bundle":"https://pith.science/pith/VSTPDRK26QU5AA72KCPIHNHT7M/bundle.json","state":"https://pith.science/pith/VSTPDRK26QU5AA72KCPIHNHT7M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VSTPDRK26QU5AA72KCPIHNHT7M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:VSTPDRK26QU5AA72KCPIHNHT7M","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":"2f5a70ae7b3fba92e9f526392dd3d1468c0359fbe9e87aadb6ac27a05fcf4573","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-15T13:56:33Z","title_canon_sha256":"5622eb998429d30e41e5b68815edbb33ee28ac4a928eddae4d0edf2a6d9159aa"},"schema_version":"1.0","source":{"id":"1710.05336","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.05336","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"arxiv_version","alias_value":"1710.05336v4","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.05336","created_at":"2026-05-18T00:24:59Z"},{"alias_kind":"pith_short_12","alias_value":"VSTPDRK26QU5","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VSTPDRK26QU5AA72","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VSTPDRK2","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:0ef6defc6414c0d71da6b05c38412c0ed1d66c0f42ee6f939b70dc953752a748","target":"graph","created_at":"2026-05-18T00:24:59Z","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 derive the off-shell nilpotent (fermionic) (anti-)BRST symmetry transformations by exploiting the (anti-)chiral superfield approach (ACSA) to Becchi-Rouet-Stora-Tyutin (BRST) formalism for the interacting Abelian 1-form gauge theories where there is a coupling between the U(1) Abelian 1-form gauge field and Dirac as well as complex scalar fields. We exploit the (anti-)BRST invariant restrictions on the (anti-)chiral superfields to derive the fermionic symmetries of our present D-dimensional Abelian 1-form gauge theories. The novel observation of our present investigation is the derivation o","authors_text":"B. Chauhan, R. P. Malik, S. Kumar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-15T13:56:33Z","title":"(Anti-)Chiral Superfield Approach to Interacting Abelian 1-Form Gauge Theories: Nilpotent and Absolutely Anticommuting Charges"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.05336","kind":"arxiv","version":4},"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":"sha256:2eb774413da0c271b4034436ae100a34e99521ca669c869878c861f4ed5b6337","target":"record","created_at":"2026-05-18T00:24:59Z","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":"2f5a70ae7b3fba92e9f526392dd3d1468c0359fbe9e87aadb6ac27a05fcf4573","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-15T13:56:33Z","title_canon_sha256":"5622eb998429d30e41e5b68815edbb33ee28ac4a928eddae4d0edf2a6d9159aa"},"schema_version":"1.0","source":{"id":"1710.05336","kind":"arxiv","version":4}},"canonical_sha256":"aca6f1c55af429d003fa509e83b4f3fb079a541b92ecddfa1709e5e08d21c626","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aca6f1c55af429d003fa509e83b4f3fb079a541b92ecddfa1709e5e08d21c626","first_computed_at":"2026-05-18T00:24:59.550574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:59.550574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gtFymS2C73mltTtBI+19pQZ4pUA0EGn0/XoffLv2BZcR9mkvYGgzjepfnwxB74tTHymn89SEWXgioCBUCn0VCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:59.551025Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.05336","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2eb774413da0c271b4034436ae100a34e99521ca669c869878c861f4ed5b6337","sha256:0ef6defc6414c0d71da6b05c38412c0ed1d66c0f42ee6f939b70dc953752a748"],"state_sha256":"2aaf12ed6cdc0ba87072d2660d08c3a1772a63b23c33700324602e9b05cc946c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g7/XXTn6fUWGdU9ggVuhwlnm5oEV2y+FxEq+a+S9k8d/k8sk2lDo1AXbQ42iK4eq8FmlTY1WIcb1a5XOLAW4DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-09T05:01:14.781848Z","bundle_sha256":"523a3653bbde856f589de14fd66b45bd0a727876dafbfbc4717be7b39a0c90be"}}