{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:DYBPLTF6YRGLDKPXWCJADARR4T","short_pith_number":"pith:DYBPLTF6","canonical_record":{"source":{"id":"hep-th/9808041","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-08-07T14:04:43Z","cross_cats_sorted":[],"title_canon_sha256":"1f5ebc498877ceddf3aec7cf7fcdc1eeaca2d2a5b2247195dd658a8691e7c942","abstract_canon_sha256":"12b6ba1ca802edb58011591807d85ca50fa6676119b29474627f4d509195f297"},"schema_version":"1.0"},"canonical_sha256":"1e02f5ccbec44cb1a9f7b092018231e4e62d7225917db5bb193d0a0a4f92a422","source":{"kind":"arxiv","id":"hep-th/9808041","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9808041","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9808041v4","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9808041","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_12","alias_value":"DYBPLTF6YRGL","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_16","alias_value":"DYBPLTF6YRGLDKPX","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_8","alias_value":"DYBPLTF6","created_at":"2026-07-04T15:38:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:DYBPLTF6YRGLDKPXWCJADARR4T","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9808041","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-08-07T14:04:43Z","cross_cats_sorted":[],"title_canon_sha256":"1f5ebc498877ceddf3aec7cf7fcdc1eeaca2d2a5b2247195dd658a8691e7c942","abstract_canon_sha256":"12b6ba1ca802edb58011591807d85ca50fa6676119b29474627f4d509195f297"},"schema_version":"1.0"},"canonical_sha256":"1e02f5ccbec44cb1a9f7b092018231e4e62d7225917db5bb193d0a0a4f92a422","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:38:27.863893Z","signature_b64":"2ERn44Wts6f7Uemye/11IBYfFBDoq+r/5QxtC0rOHSyifABNw+UazMJZhSf6jdzq8tj/Aan5tNz0gkl/SsXoCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e02f5ccbec44cb1a9f7b092018231e4e62d7225917db5bb193d0a0a4f92a422","last_reissued_at":"2026-07-04T15:38:27.863498Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:38:27.863498Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9808041","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":"2026-07-04T15:38:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"El31ezWEAD1HkzatTPjPGCB9gaq7fQLsut54pxM8+C9YwkLYuEihIrxfmrFDR8SM3T4IHncYiyM5zUtmzLQPAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T14:36:18.489993Z"},"content_sha256":"e52e964a71c919b622b53ee3d93bacb5ee99f112d5f4d1cd1f7e954c2b07f686","schema_version":"1.0","event_id":"sha256:e52e964a71c919b622b53ee3d93bacb5ee99f112d5f4d1cd1f7e954c2b07f686"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:DYBPLTF6YRGLDKPXWCJADARR4T","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"N=1 Superconformal Symmetry in Four Dimensional Quantum Field Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Hugh Osborn","submitted_at":"1998-08-07T14:04:43Z","abstract_excerpt":"The implications of N=1 superconformal symmetry for four dimensional quantum field theories are studied. Superconformal covariant expressions for two and three point functions of quasi-primary superfields of arbitrary spin are found and connected with the operator product expansion. The general formulae are specialised to cases involving a scalar superfield L, which contains global symmetry currents, and the supercurrent, which contains the energy momentum tensor, and the consequences of superconformal Ward identities analysed. The three point function of L is shown to have unique completely a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9808041","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9808041/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:38:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3ZK3wNBGjhhjWduxfeA6nUtkMoUL/8RSkLjvTKh2MtWc9sJXPp98EAvfIIiWvT7abLHWGYNAosOvZ5C+healAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T14:36:18.490571Z"},"content_sha256":"5e79d6fad0e21489ce97182546681b4b970fbfa7194c7b314a90c2325d308f1a","schema_version":"1.0","event_id":"sha256:5e79d6fad0e21489ce97182546681b4b970fbfa7194c7b314a90c2325d308f1a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DYBPLTF6YRGLDKPXWCJADARR4T/bundle.json","state_url":"https://pith.science/pith/DYBPLTF6YRGLDKPXWCJADARR4T/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DYBPLTF6YRGLDKPXWCJADARR4T/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":"2026-08-08T14:36:18Z","links":{"resolver":"https://pith.science/pith/DYBPLTF6YRGLDKPXWCJADARR4T","bundle":"https://pith.science/pith/DYBPLTF6YRGLDKPXWCJADARR4T/bundle.json","state":"https://pith.science/pith/DYBPLTF6YRGLDKPXWCJADARR4T/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DYBPLTF6YRGLDKPXWCJADARR4T/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:DYBPLTF6YRGLDKPXWCJADARR4T","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":"12b6ba1ca802edb58011591807d85ca50fa6676119b29474627f4d509195f297","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-08-07T14:04:43Z","title_canon_sha256":"1f5ebc498877ceddf3aec7cf7fcdc1eeaca2d2a5b2247195dd658a8691e7c942"},"schema_version":"1.0","source":{"id":"hep-th/9808041","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9808041","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9808041v4","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9808041","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_12","alias_value":"DYBPLTF6YRGL","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_16","alias_value":"DYBPLTF6YRGLDKPX","created_at":"2026-07-04T15:38:27Z"},{"alias_kind":"pith_short_8","alias_value":"DYBPLTF6","created_at":"2026-07-04T15:38:27Z"}],"graph_snapshots":[{"event_id":"sha256:5e79d6fad0e21489ce97182546681b4b970fbfa7194c7b314a90c2325d308f1a","target":"graph","created_at":"2026-07-04T15:38:27Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9808041/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The implications of N=1 superconformal symmetry for four dimensional quantum field theories are studied. Superconformal covariant expressions for two and three point functions of quasi-primary superfields of arbitrary spin are found and connected with the operator product expansion. The general formulae are specialised to cases involving a scalar superfield L, which contains global symmetry currents, and the supercurrent, which contains the energy momentum tensor, and the consequences of superconformal Ward identities analysed. The three point function of L is shown to have unique completely a","authors_text":"Hugh Osborn","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1998-08-07T14:04:43Z","title":"N=1 Superconformal Symmetry in Four Dimensional Quantum Field Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9808041","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:e52e964a71c919b622b53ee3d93bacb5ee99f112d5f4d1cd1f7e954c2b07f686","target":"record","created_at":"2026-07-04T15:38:27Z","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":"12b6ba1ca802edb58011591807d85ca50fa6676119b29474627f4d509195f297","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-08-07T14:04:43Z","title_canon_sha256":"1f5ebc498877ceddf3aec7cf7fcdc1eeaca2d2a5b2247195dd658a8691e7c942"},"schema_version":"1.0","source":{"id":"hep-th/9808041","kind":"arxiv","version":4}},"canonical_sha256":"1e02f5ccbec44cb1a9f7b092018231e4e62d7225917db5bb193d0a0a4f92a422","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1e02f5ccbec44cb1a9f7b092018231e4e62d7225917db5bb193d0a0a4f92a422","first_computed_at":"2026-07-04T15:38:27.863498Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:38:27.863498Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2ERn44Wts6f7Uemye/11IBYfFBDoq+r/5QxtC0rOHSyifABNw+UazMJZhSf6jdzq8tj/Aan5tNz0gkl/SsXoCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:38:27.863893Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9808041","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e52e964a71c919b622b53ee3d93bacb5ee99f112d5f4d1cd1f7e954c2b07f686","sha256:5e79d6fad0e21489ce97182546681b4b970fbfa7194c7b314a90c2325d308f1a"],"state_sha256":"09af8862775314c95fe18a6ea8895b21af2e42670c96ac9205a877f8f2ec7c2a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eolWybqGDeIMcnZiYArj9huDdJqIvo3fRH64IJT0dFZ9TqF3T6oDFiWoKF5ljJSWFNDLmezMfTho5Nhj7zdjDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T14:36:18.494927Z","bundle_sha256":"7b91768c24aeada6cd89ebca39da6446f939357b5d356e1ecd9407e3169b517b"}}