{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:LZQHQPJOSMZ6XAGR4IV3N5ADRH","short_pith_number":"pith:LZQHQPJO","canonical_record":{"source":{"id":"hep-th/9802097","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-02-13T09:50:51Z","cross_cats_sorted":[],"title_canon_sha256":"6976ba1c9f1e9fe1c23bf47a7144311950a793bae9cd3bdd5211ffa9089f3e34","abstract_canon_sha256":"32c2fe9ef5b46fd6731bcc98bc9c72a892156ee3cc20c72df2b2e850a9aea847"},"schema_version":"1.0"},"canonical_sha256":"5e60783d2e9333eb80d1e22bb6f40389f45d99cc37e36106aa8a52cf1a866a0f","source":{"kind":"arxiv","id":"hep-th/9802097","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9802097","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9802097v1","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9802097","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_12","alias_value":"LZQHQPJOSMZ6","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_16","alias_value":"LZQHQPJOSMZ6XAGR","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_8","alias_value":"LZQHQPJO","created_at":"2026-07-04T16:09:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:LZQHQPJOSMZ6XAGR4IV3N5ADRH","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9802097","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-02-13T09:50:51Z","cross_cats_sorted":[],"title_canon_sha256":"6976ba1c9f1e9fe1c23bf47a7144311950a793bae9cd3bdd5211ffa9089f3e34","abstract_canon_sha256":"32c2fe9ef5b46fd6731bcc98bc9c72a892156ee3cc20c72df2b2e850a9aea847"},"schema_version":"1.0"},"canonical_sha256":"5e60783d2e9333eb80d1e22bb6f40389f45d99cc37e36106aa8a52cf1a866a0f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:41.508198Z","signature_b64":"a6M4k8HvkT6ztenEhJuuHts0Hq8ll7k7ON3g58WFLVa4LTLhdhy30o7gNTGyrA+0viwYDKd3Xg82JqAmd4VoBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e60783d2e9333eb80d1e22bb6f40389f45d99cc37e36106aa8a52cf1a866a0f","last_reissued_at":"2026-07-04T16:09:41.507849Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:41.507849Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9802097","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":"2026-07-04T16:09:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qlikS5b29V3D93BzBaGA/V17V/K58GJZNu8jKe/qXs6pRh8i4O337D2JVI7oof5rd+TaizLWeLg9u58r7TbZCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T20:49:34.104108Z"},"content_sha256":"577314c3eff3ec19bda923a68984192a254628056cafbc02d32d532c72e14b97","schema_version":"1.0","event_id":"sha256:577314c3eff3ec19bda923a68984192a254628056cafbc02d32d532c72e14b97"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:LZQHQPJOSMZ6XAGR4IV3N5ADRH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fermionic fields in the d-dimensional anti-de Sitter spacetime","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R.R.Metsaev (Lebedev Physical Institute)","submitted_at":"1998-02-13T09:50:51Z","abstract_excerpt":"Arbitrary spin free massless fermionic fields corresponding to mixed symmetry representations of the \\hbox{$SO(d-1)$} compact group and propagating in even $d$-dimensional anti-de Sitter spacetime are investigated. Free wave equations of motion, subsidiary conditions and the corresponding gauge transformations for such fields are proposed. The lowest eigenvalues of the energy operator for the massless fields and the gauge parameter fields are derived. The results are formulated in $SO(d-1,2)$ covariant form as well as in terms of intrinsic coordinates."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9802097","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9802097/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":"2026-07-04T16:09:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l5RHWG4zezb3w/gFl5T/oVmUQAV3JUTCBPYiNFyaNPgxJ8op6IsGSWi7EjdKQdLZUG0gSEFxh3DxTLKNUHCtBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T20:49:34.104593Z"},"content_sha256":"4e0c2ab85946e6246f6284c1b9c29fb897667971ea21ee2066ce5a9113d03243","schema_version":"1.0","event_id":"sha256:4e0c2ab85946e6246f6284c1b9c29fb897667971ea21ee2066ce5a9113d03243"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/bundle.json","state_url":"https://pith.science/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/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":"2026-08-11T20:49:34Z","links":{"resolver":"https://pith.science/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH","bundle":"https://pith.science/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/bundle.json","state":"https://pith.science/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LZQHQPJOSMZ6XAGR4IV3N5ADRH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:LZQHQPJOSMZ6XAGR4IV3N5ADRH","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":"32c2fe9ef5b46fd6731bcc98bc9c72a892156ee3cc20c72df2b2e850a9aea847","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-02-13T09:50:51Z","title_canon_sha256":"6976ba1c9f1e9fe1c23bf47a7144311950a793bae9cd3bdd5211ffa9089f3e34"},"schema_version":"1.0","source":{"id":"hep-th/9802097","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9802097","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9802097v1","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9802097","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_12","alias_value":"LZQHQPJOSMZ6","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_16","alias_value":"LZQHQPJOSMZ6XAGR","created_at":"2026-07-04T16:09:41Z"},{"alias_kind":"pith_short_8","alias_value":"LZQHQPJO","created_at":"2026-07-04T16:09:41Z"}],"graph_snapshots":[{"event_id":"sha256:4e0c2ab85946e6246f6284c1b9c29fb897667971ea21ee2066ce5a9113d03243","target":"graph","created_at":"2026-07-04T16:09:41Z","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/9802097/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Arbitrary spin free massless fermionic fields corresponding to mixed symmetry representations of the \\hbox{$SO(d-1)$} compact group and propagating in even $d$-dimensional anti-de Sitter spacetime are investigated. Free wave equations of motion, subsidiary conditions and the corresponding gauge transformations for such fields are proposed. The lowest eigenvalues of the energy operator for the massless fields and the gauge parameter fields are derived. The results are formulated in $SO(d-1,2)$ covariant form as well as in terms of intrinsic coordinates.","authors_text":"R.R.Metsaev (Lebedev Physical Institute)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1998-02-13T09:50:51Z","title":"Fermionic fields in the d-dimensional anti-de Sitter spacetime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9802097","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":"sha256:577314c3eff3ec19bda923a68984192a254628056cafbc02d32d532c72e14b97","target":"record","created_at":"2026-07-04T16:09:41Z","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":"32c2fe9ef5b46fd6731bcc98bc9c72a892156ee3cc20c72df2b2e850a9aea847","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-02-13T09:50:51Z","title_canon_sha256":"6976ba1c9f1e9fe1c23bf47a7144311950a793bae9cd3bdd5211ffa9089f3e34"},"schema_version":"1.0","source":{"id":"hep-th/9802097","kind":"arxiv","version":1}},"canonical_sha256":"5e60783d2e9333eb80d1e22bb6f40389f45d99cc37e36106aa8a52cf1a866a0f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5e60783d2e9333eb80d1e22bb6f40389f45d99cc37e36106aa8a52cf1a866a0f","first_computed_at":"2026-07-04T16:09:41.507849Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:09:41.507849Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a6M4k8HvkT6ztenEhJuuHts0Hq8ll7k7ON3g58WFLVa4LTLhdhy30o7gNTGyrA+0viwYDKd3Xg82JqAmd4VoBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:09:41.508198Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9802097","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:577314c3eff3ec19bda923a68984192a254628056cafbc02d32d532c72e14b97","sha256:4e0c2ab85946e6246f6284c1b9c29fb897667971ea21ee2066ce5a9113d03243"],"state_sha256":"eb829bc06f58b8e25fe58d1e2d941fd110451f7ac0422dbfbe2bd22b72651353"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oOSwAs4zFTlp5qF15m3+vDvhPxWYi5A3DHn9Y3U8+UE/72ePlLgkAhUupnMEQQjHinVcyMId3TczFhWy5qr+AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T20:49:34.109032Z","bundle_sha256":"de3a4f84a2a2e689968c9f32d22ed52475d95c7182aa184bb3003fee0b86e9a5"}}