{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:EMY7LFCQWCFSKEMSYFNVVR26S6","short_pith_number":"pith:EMY7LFCQ","canonical_record":{"source":{"id":"hep-th/0609029","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-09-04T18:48:34Z","cross_cats_sorted":[],"title_canon_sha256":"5ebe686442846411b5eff0e41d5d4310131c5472aca1bb7e8fe4e3d070f474cc","abstract_canon_sha256":"8055bc816a2ccf87530b12d4b906ba901b23c39acd9e3a7b70c49eedc50fd49b"},"schema_version":"1.0"},"canonical_sha256":"2331f59450b08b251192c15b5ac75e97aa8f9a52ec8e5be2e5c882a9ed3faa16","source":{"kind":"arxiv","id":"hep-th/0609029","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0609029","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0609029v3","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0609029","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_12","alias_value":"EMY7LFCQWCFS","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_16","alias_value":"EMY7LFCQWCFSKEMS","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_8","alias_value":"EMY7LFCQ","created_at":"2026-07-04T15:17:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:EMY7LFCQWCFSKEMSYFNVVR26S6","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0609029","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-09-04T18:48:34Z","cross_cats_sorted":[],"title_canon_sha256":"5ebe686442846411b5eff0e41d5d4310131c5472aca1bb7e8fe4e3d070f474cc","abstract_canon_sha256":"8055bc816a2ccf87530b12d4b906ba901b23c39acd9e3a7b70c49eedc50fd49b"},"schema_version":"1.0"},"canonical_sha256":"2331f59450b08b251192c15b5ac75e97aa8f9a52ec8e5be2e5c882a9ed3faa16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:14.202202Z","signature_b64":"gCcOB6FMF+V9p77o49ntdqSzkY3sc5ty8chiz+oKszzOHZxTlaa4a6QjtqeV6FpQsunccv+xXyK+r4/yZMceBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2331f59450b08b251192c15b5ac75e97aa8f9a52ec8e5be2e5c882a9ed3faa16","last_reissued_at":"2026-07-04T15:17:14.201792Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:14.201792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0609029","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":"2026-07-04T15:17:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ni9o6RPIKO8pQzQVsvrqRNUXHJnEqINlIDPX5xQAhwxpUxN/4N4sbY0zKb9fXrUaiJHnc55UpwT5g3cq//AyAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T09:10:41.747446Z"},"content_sha256":"f9bf77632d15a9dc3eadc24484fb80f81c29cf085d29e3e93de0c86d813761fa","schema_version":"1.0","event_id":"sha256:f9bf77632d15a9dc3eadc24484fb80f81c29cf085d29e3e93de0c86d813761fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:EMY7LFCQWCFSKEMSYFNVVR26S6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gauge invariant formulation of massive totally symmetric fermionic fields in (A)dS space","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R. R. Metsaev","submitted_at":"2006-09-04T18:48:34Z","abstract_excerpt":"Massive arbitrary spin totally symmetric free fermionic fields propagating in d-dimensional (Anti)-de Sitter space-time are investigated. Gauge invariant action and the corresponding gauge transformations for such fields are proposed. The results are formulated in terms of various mass parameters used in the literature as well as the lowest eigenvalues of the energy operator. We apply our results to a study of partial masslessness of fermionic fields in (A)dS(d), and in the case of d=4 confirm the conjecture made in the earlier literature."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0609029","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/0609029/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":"2026-07-04T15:17:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RfCXBBXspP48982S/6yFatmrGC/+GmcajO2RnVJcugWkkiIhlZZ4CA8wexHCsKGaM16caPyV2/7dYUgS7220Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T09:10:41.747980Z"},"content_sha256":"716c3a7fa07fd1850422aef22c910d319810c658b2c82e68aa218ddd7463b2b2","schema_version":"1.0","event_id":"sha256:716c3a7fa07fd1850422aef22c910d319810c658b2c82e68aa218ddd7463b2b2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/bundle.json","state_url":"https://pith.science/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/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":"2026-08-12T09:10:41Z","links":{"resolver":"https://pith.science/pith/EMY7LFCQWCFSKEMSYFNVVR26S6","bundle":"https://pith.science/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/bundle.json","state":"https://pith.science/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EMY7LFCQWCFSKEMSYFNVVR26S6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:EMY7LFCQWCFSKEMSYFNVVR26S6","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":"8055bc816a2ccf87530b12d4b906ba901b23c39acd9e3a7b70c49eedc50fd49b","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2006-09-04T18:48:34Z","title_canon_sha256":"5ebe686442846411b5eff0e41d5d4310131c5472aca1bb7e8fe4e3d070f474cc"},"schema_version":"1.0","source":{"id":"hep-th/0609029","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0609029","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0609029v3","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0609029","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_12","alias_value":"EMY7LFCQWCFS","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_16","alias_value":"EMY7LFCQWCFSKEMS","created_at":"2026-07-04T15:17:14Z"},{"alias_kind":"pith_short_8","alias_value":"EMY7LFCQ","created_at":"2026-07-04T15:17:14Z"}],"graph_snapshots":[{"event_id":"sha256:716c3a7fa07fd1850422aef22c910d319810c658b2c82e68aa218ddd7463b2b2","target":"graph","created_at":"2026-07-04T15:17:14Z","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/0609029/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Massive arbitrary spin totally symmetric free fermionic fields propagating in d-dimensional (Anti)-de Sitter space-time are investigated. Gauge invariant action and the corresponding gauge transformations for such fields are proposed. The results are formulated in terms of various mass parameters used in the literature as well as the lowest eigenvalues of the energy operator. We apply our results to a study of partial masslessness of fermionic fields in (A)dS(d), and in the case of d=4 confirm the conjecture made in the earlier literature.","authors_text":"R. R. Metsaev","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2006-09-04T18:48:34Z","title":"Gauge invariant formulation of massive totally symmetric fermionic fields in (A)dS space"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0609029","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:f9bf77632d15a9dc3eadc24484fb80f81c29cf085d29e3e93de0c86d813761fa","target":"record","created_at":"2026-07-04T15:17:14Z","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":"8055bc816a2ccf87530b12d4b906ba901b23c39acd9e3a7b70c49eedc50fd49b","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2006-09-04T18:48:34Z","title_canon_sha256":"5ebe686442846411b5eff0e41d5d4310131c5472aca1bb7e8fe4e3d070f474cc"},"schema_version":"1.0","source":{"id":"hep-th/0609029","kind":"arxiv","version":3}},"canonical_sha256":"2331f59450b08b251192c15b5ac75e97aa8f9a52ec8e5be2e5c882a9ed3faa16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2331f59450b08b251192c15b5ac75e97aa8f9a52ec8e5be2e5c882a9ed3faa16","first_computed_at":"2026-07-04T15:17:14.201792Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:17:14.201792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gCcOB6FMF+V9p77o49ntdqSzkY3sc5ty8chiz+oKszzOHZxTlaa4a6QjtqeV6FpQsunccv+xXyK+r4/yZMceBA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:17:14.202202Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0609029","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f9bf77632d15a9dc3eadc24484fb80f81c29cf085d29e3e93de0c86d813761fa","sha256:716c3a7fa07fd1850422aef22c910d319810c658b2c82e68aa218ddd7463b2b2"],"state_sha256":"abf50ec88420ce6a98eae30a69ae811fb8982558ffd1ad56dad01a6b4604d2c8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l7EKqn+30AJhcJZCRT2Lr+RxL1/kiYsoJDii16m0sjaeEey45/CuHVBcyyrV/D4l8JKqyV2hDnRFmMo1z05yCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T09:10:41.752227Z","bundle_sha256":"3a99660ca5b3acf612c0ff973680944558d83316481fd682c0e4a2a377c579d8"}}