{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1999:QFIFO5MCZPRGLMM6K2RZ3S2X3Q","short_pith_number":"pith:QFIFO5MC","canonical_record":{"source":{"id":"hep-th/9906077","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-06-10T20:47:05Z","cross_cats_sorted":[],"title_canon_sha256":"6382c1c788a0c8d554e8347fa067e2fd7cd69e2178002b4bb72d42fcf3052466","abstract_canon_sha256":"62304965798270e8cc02b26800b11f8d99e1c36806cd18fee80c19503b2ca99f"},"schema_version":"1.0"},"canonical_sha256":"8150577582cbe265b19e56a39dcb57dc3480d2d04c9e70f717a0186930c87a3b","source":{"kind":"arxiv","id":"hep-th/9906077","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9906077","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9906077v3","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9906077","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_12","alias_value":"QFIFO5MCZPRG","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_16","alias_value":"QFIFO5MCZPRGLMM6","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_8","alias_value":"QFIFO5MC","created_at":"2026-07-04T16:14:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1999:QFIFO5MCZPRGLMM6K2RZ3S2X3Q","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9906077","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-06-10T20:47:05Z","cross_cats_sorted":[],"title_canon_sha256":"6382c1c788a0c8d554e8347fa067e2fd7cd69e2178002b4bb72d42fcf3052466","abstract_canon_sha256":"62304965798270e8cc02b26800b11f8d99e1c36806cd18fee80c19503b2ca99f"},"schema_version":"1.0"},"canonical_sha256":"8150577582cbe265b19e56a39dcb57dc3480d2d04c9e70f717a0186930c87a3b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:52.159937Z","signature_b64":"s0uq5yM4FkWUY8XidAHrZIrlECCngADqFrQ3tyn/YjdYpQtwQi/GdDBtEIy/u24ZKisDvNtQZW7AJxAln8POBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8150577582cbe265b19e56a39dcb57dc3480d2d04c9e70f717a0186930c87a3b","last_reissued_at":"2026-07-04T16:14:52.159565Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:52.159565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9906077","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":"2026-07-04T16:14:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JP4O3Fh92z9tMMgh81E68ki12GWwo38+Ulcb/2BpXyZi1eDDF63kJ9TdwtDsmA6bBp2pjOkmivtXHUyWjmQtDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T13:40:40.419182Z"},"content_sha256":"76df25d79b8d5d76933807e4663a4d1be460be3806e89a6cbfe23e7d2eb24226","schema_version":"1.0","event_id":"sha256:76df25d79b8d5d76933807e4663a4d1be460be3806e89a6cbfe23e7d2eb24226"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1999:QFIFO5MCZPRGLMM6K2RZ3S2X3Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The AdS/CFT Correspondence for the Massive Rarita-Schwinger Field","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"K. S. Viswanathan, P. Matlock","submitted_at":"1999-06-10T20:47:05Z","abstract_excerpt":"The complete solution to the massive Rarita-Schwinger field equation in anti-de Sitter space is constructed, and used in the AdS/CFT correspondence to calculate the correlators for the boundary conformal field theory. It is found that when no condition is imposed on the field solution, there appear two different boundary conformal field operators, one coupling to a Rarita-Schwinger field and the other to a Dirac field. These two operators are seen to have different scaling dimensions, with that of the spinor-coupled operator exhibiting non-analytic mass dependence."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9906077","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9906077/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":"2026-07-04T16:14:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dtEiG0SkNFLD/2G++Wx1jWSOURroFBMKSTjpJJJ6JXlIJ+EurvHonhBp2tljqzsT1OexCNXmw6yqTAuaKo/qBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T13:40:40.419690Z"},"content_sha256":"39f503182d16ecd2d0300dca8bcff9daecb89fe5bcdced4cbc203c4641d513a9","schema_version":"1.0","event_id":"sha256:39f503182d16ecd2d0300dca8bcff9daecb89fe5bcdced4cbc203c4641d513a9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/bundle.json","state_url":"https://pith.science/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/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":"2026-08-05T13:40:40Z","links":{"resolver":"https://pith.science/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q","bundle":"https://pith.science/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/bundle.json","state":"https://pith.science/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QFIFO5MCZPRGLMM6K2RZ3S2X3Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1999:QFIFO5MCZPRGLMM6K2RZ3S2X3Q","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":"62304965798270e8cc02b26800b11f8d99e1c36806cd18fee80c19503b2ca99f","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1999-06-10T20:47:05Z","title_canon_sha256":"6382c1c788a0c8d554e8347fa067e2fd7cd69e2178002b4bb72d42fcf3052466"},"schema_version":"1.0","source":{"id":"hep-th/9906077","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9906077","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9906077v3","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9906077","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_12","alias_value":"QFIFO5MCZPRG","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_16","alias_value":"QFIFO5MCZPRGLMM6","created_at":"2026-07-04T16:14:52Z"},{"alias_kind":"pith_short_8","alias_value":"QFIFO5MC","created_at":"2026-07-04T16:14:52Z"}],"graph_snapshots":[{"event_id":"sha256:39f503182d16ecd2d0300dca8bcff9daecb89fe5bcdced4cbc203c4641d513a9","target":"graph","created_at":"2026-07-04T16:14:52Z","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/9906077/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The complete solution to the massive Rarita-Schwinger field equation in anti-de Sitter space is constructed, and used in the AdS/CFT correspondence to calculate the correlators for the boundary conformal field theory. It is found that when no condition is imposed on the field solution, there appear two different boundary conformal field operators, one coupling to a Rarita-Schwinger field and the other to a Dirac field. These two operators are seen to have different scaling dimensions, with that of the spinor-coupled operator exhibiting non-analytic mass dependence.","authors_text":"K. S. Viswanathan, P. Matlock","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1999-06-10T20:47:05Z","title":"The AdS/CFT Correspondence for the Massive Rarita-Schwinger Field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9906077","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":"sha256:76df25d79b8d5d76933807e4663a4d1be460be3806e89a6cbfe23e7d2eb24226","target":"record","created_at":"2026-07-04T16:14:52Z","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":"62304965798270e8cc02b26800b11f8d99e1c36806cd18fee80c19503b2ca99f","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1999-06-10T20:47:05Z","title_canon_sha256":"6382c1c788a0c8d554e8347fa067e2fd7cd69e2178002b4bb72d42fcf3052466"},"schema_version":"1.0","source":{"id":"hep-th/9906077","kind":"arxiv","version":3}},"canonical_sha256":"8150577582cbe265b19e56a39dcb57dc3480d2d04c9e70f717a0186930c87a3b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8150577582cbe265b19e56a39dcb57dc3480d2d04c9e70f717a0186930c87a3b","first_computed_at":"2026-07-04T16:14:52.159565Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:14:52.159565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"s0uq5yM4FkWUY8XidAHrZIrlECCngADqFrQ3tyn/YjdYpQtwQi/GdDBtEIy/u24ZKisDvNtQZW7AJxAln8POBg==","signature_status":"signed_v1","signed_at":"2026-07-04T16:14:52.159937Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9906077","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:76df25d79b8d5d76933807e4663a4d1be460be3806e89a6cbfe23e7d2eb24226","sha256:39f503182d16ecd2d0300dca8bcff9daecb89fe5bcdced4cbc203c4641d513a9"],"state_sha256":"c8781c3fce3621ca2c0a13751c0dd934e8535fdb0ef5c5f3d8c4fa3f14c48e34"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bnc2TmfPIlHd7WxVbhnKuwSBluXmFYKy7Z6CD+FFDTbrI5uvknxA71Qp8lIkdMGbDH/ABLzPJ5r6ilg7prjICQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T13:40:40.423950Z","bundle_sha256":"87d91039b29feae17f7b300b515e41dd89c477c3faaa7f5327a8ccb14948b7b4"}}