{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:C4I5WBTVUEXD6MJLH2IF67VFIB","short_pith_number":"pith:C4I5WBTV","canonical_record":{"source":{"id":"1703.05780","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-16T18:09:46Z","cross_cats_sorted":[],"title_canon_sha256":"62586ba2c60d867aa2aead73f5584b954ca12d9bb46a722bea49fd005bce0352","abstract_canon_sha256":"e799c525bfd47551ef5901c3abdcc6dfe601383bea7066f8adacc67a4d716bce"},"schema_version":"1.0"},"canonical_sha256":"1711db0675a12e3f312b3e905f7ea5405ef94554e451ddbbbe68f9e32ea11360","source":{"kind":"arxiv","id":"1703.05780","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.05780","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"arxiv_version","alias_value":"1703.05780v2","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05780","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"pith_short_12","alias_value":"C4I5WBTVUEXD","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"C4I5WBTVUEXD6MJL","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"C4I5WBTV","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:C4I5WBTVUEXD6MJLH2IF67VFIB","target":"record","payload":{"canonical_record":{"source":{"id":"1703.05780","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-16T18:09:46Z","cross_cats_sorted":[],"title_canon_sha256":"62586ba2c60d867aa2aead73f5584b954ca12d9bb46a722bea49fd005bce0352","abstract_canon_sha256":"e799c525bfd47551ef5901c3abdcc6dfe601383bea7066f8adacc67a4d716bce"},"schema_version":"1.0"},"canonical_sha256":"1711db0675a12e3f312b3e905f7ea5405ef94554e451ddbbbe68f9e32ea11360","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:39.325890Z","signature_b64":"PZZNCFuXpr5Hwex0DTG/NDqG661+nmaZKqUdEyaF0NoIYaQAoyjfoH2GeRwRlJ77WRm2sEkMp1EqjBMXsI7tDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1711db0675a12e3f312b3e905f7ea5405ef94554e451ddbbbe68f9e32ea11360","last_reissued_at":"2026-05-18T00:33:39.325407Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:39.325407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.05780","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:33:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wVBTPfUGY8z6ZAK0r64k3VZ5N1QWFQmuAKEM3NeTIe+uQi9ko0x4DTc+uUQAbwyJVYdDYUnDwHUQ5wdwV+irCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T13:00:51.830118Z"},"content_sha256":"4d3be54f8b3c40852ed7e1de8e67af4005d57aa8fec7a2789e61240077eb22a7","schema_version":"1.0","event_id":"sha256:4d3be54f8b3c40852ed7e1de8e67af4005d57aa8fec7a2789e61240077eb22a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:C4I5WBTVUEXD6MJLH2IF67VFIB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fermionic continuous spin gauge field in (A)dS space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R.R. Metsaev","submitted_at":"2017-03-16T18:09:46Z","abstract_excerpt":"Fermionic continuous spin field propagating in (A)dS space-time is studied. Gauge invariant Lagrangian formulation for such fermionic field is developed. Lagrangian of the fermionic continuous spin field is constructed in terms of triple gamma-traceless tensor-spinor Dirac fields, while gauge symmetries are realized by using gamma-traceless gauge transformation parameters. It is demonstrated that partition function of fermionic continuous spin field is equal to one. Modified de Donder gauge condition that considerably simplifies analysis of equations of motion is found. Decoupling limits leadi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05780","kind":"arxiv","version":2},"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":"2026-05-18T00:33:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8ax4vrChmqEu9AgSxHjJHevpCNqrzi9adj1A28IVPhNnbOdhYt9O/m77QezOvEKbQ6QMnIJX2T0B3vYHWwjcCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T13:00:51.830675Z"},"content_sha256":"ba7ce0b01b0389544fda3a55f7188a713438b5903fde05c6c3831c80836b4556","schema_version":"1.0","event_id":"sha256:ba7ce0b01b0389544fda3a55f7188a713438b5903fde05c6c3831c80836b4556"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/bundle.json","state_url":"https://pith.science/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/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":"2026-05-20T13:00:51Z","links":{"resolver":"https://pith.science/pith/C4I5WBTVUEXD6MJLH2IF67VFIB","bundle":"https://pith.science/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/bundle.json","state":"https://pith.science/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C4I5WBTVUEXD6MJLH2IF67VFIB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:C4I5WBTVUEXD6MJLH2IF67VFIB","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":"e799c525bfd47551ef5901c3abdcc6dfe601383bea7066f8adacc67a4d716bce","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-16T18:09:46Z","title_canon_sha256":"62586ba2c60d867aa2aead73f5584b954ca12d9bb46a722bea49fd005bce0352"},"schema_version":"1.0","source":{"id":"1703.05780","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.05780","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"arxiv_version","alias_value":"1703.05780v2","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05780","created_at":"2026-05-18T00:33:39Z"},{"alias_kind":"pith_short_12","alias_value":"C4I5WBTVUEXD","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"C4I5WBTVUEXD6MJL","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"C4I5WBTV","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:ba7ce0b01b0389544fda3a55f7188a713438b5903fde05c6c3831c80836b4556","target":"graph","created_at":"2026-05-18T00:33:39Z","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":"Fermionic continuous spin field propagating in (A)dS space-time is studied. Gauge invariant Lagrangian formulation for such fermionic field is developed. Lagrangian of the fermionic continuous spin field is constructed in terms of triple gamma-traceless tensor-spinor Dirac fields, while gauge symmetries are realized by using gamma-traceless gauge transformation parameters. It is demonstrated that partition function of fermionic continuous spin field is equal to one. Modified de Donder gauge condition that considerably simplifies analysis of equations of motion is found. Decoupling limits leadi","authors_text":"R.R. Metsaev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-16T18:09:46Z","title":"Fermionic continuous spin gauge field in (A)dS space"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05780","kind":"arxiv","version":2},"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":"sha256:4d3be54f8b3c40852ed7e1de8e67af4005d57aa8fec7a2789e61240077eb22a7","target":"record","created_at":"2026-05-18T00:33:39Z","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":"e799c525bfd47551ef5901c3abdcc6dfe601383bea7066f8adacc67a4d716bce","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-16T18:09:46Z","title_canon_sha256":"62586ba2c60d867aa2aead73f5584b954ca12d9bb46a722bea49fd005bce0352"},"schema_version":"1.0","source":{"id":"1703.05780","kind":"arxiv","version":2}},"canonical_sha256":"1711db0675a12e3f312b3e905f7ea5405ef94554e451ddbbbe68f9e32ea11360","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1711db0675a12e3f312b3e905f7ea5405ef94554e451ddbbbe68f9e32ea11360","first_computed_at":"2026-05-18T00:33:39.325407Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:39.325407Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PZZNCFuXpr5Hwex0DTG/NDqG661+nmaZKqUdEyaF0NoIYaQAoyjfoH2GeRwRlJ77WRm2sEkMp1EqjBMXsI7tDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:39.325890Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.05780","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4d3be54f8b3c40852ed7e1de8e67af4005d57aa8fec7a2789e61240077eb22a7","sha256:ba7ce0b01b0389544fda3a55f7188a713438b5903fde05c6c3831c80836b4556"],"state_sha256":"5497e447ccec4ab56062bacf9bdfeba89575091448de8949c5fe89054e79d182"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"A4F4nv3O0xriDGAdI6kPmvY+poqGvTAcXGh0KhNIN79XYEJk083Reo9o3ASDwCy2KuOcUEoOz6x8P/7ay4NvBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T13:00:51.833394Z","bundle_sha256":"d81b259e9e18e52829b89b03e68f09cc334dbcb714aa69f6664c428df2a0bb28"}}