{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:AIZPN6XEFO3KFRNQE3C5AZIP66","short_pith_number":"pith:AIZPN6XE","canonical_record":{"source":{"id":"1707.08832","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-27T12:26:45Z","cross_cats_sorted":[],"title_canon_sha256":"8fcc8fba1031f6f789e8283da358f943d56fa8c88c156b5c8560e2b612a5ee96","abstract_canon_sha256":"a68fdd479220a94f133da3299be674e9285766a495d21367029c040bbcbe9ea7"},"schema_version":"1.0"},"canonical_sha256":"0232f6fae42bb6a2c5b026c5d0650ff790aee142315679fdb5f5cb2f9e2c95ea","source":{"kind":"arxiv","id":"1707.08832","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.08832","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"arxiv_version","alias_value":"1707.08832v1","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.08832","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"pith_short_12","alias_value":"AIZPN6XEFO3K","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AIZPN6XEFO3KFRNQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AIZPN6XE","created_at":"2026-05-18T12:31:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:AIZPN6XEFO3KFRNQE3C5AZIP66","target":"record","payload":{"canonical_record":{"source":{"id":"1707.08832","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-27T12:26:45Z","cross_cats_sorted":[],"title_canon_sha256":"8fcc8fba1031f6f789e8283da358f943d56fa8c88c156b5c8560e2b612a5ee96","abstract_canon_sha256":"a68fdd479220a94f133da3299be674e9285766a495d21367029c040bbcbe9ea7"},"schema_version":"1.0"},"canonical_sha256":"0232f6fae42bb6a2c5b026c5d0650ff790aee142315679fdb5f5cb2f9e2c95ea","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:30.205893Z","signature_b64":"a8GKVXOmEiiJpzcRhrUNGyunqidI8yq/Se8sJ39oyrbuYiKfweOE2uahZAnmIEzUU6JPaK3BR/aGkC/Rt1kpCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0232f6fae42bb6a2c5b026c5d0650ff790aee142315679fdb5f5cb2f9e2c95ea","last_reissued_at":"2026-05-18T00:30:30.205299Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:30.205299Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.08832","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":"2026-05-18T00:30:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KjVe2u2JY3OcU4QbE15XJKEexPnzDOKcqqwqEjksOjR4OmN0S6qMikr6lzv1jiRUp8bUr8mMcIQGZOLW5W++DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:30:54.415528Z"},"content_sha256":"046dd3e0380c02ddc7ecb9df18ffaaf7a6966370b2c655cedb10657d68996540","schema_version":"1.0","event_id":"sha256:046dd3e0380c02ddc7ecb9df18ffaaf7a6966370b2c655cedb10657d68996540"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:AIZPN6XEFO3KFRNQE3C5AZIP66","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Infinite spin fields in d = 3 and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Yu. M. Zinoviev","submitted_at":"2017-07-27T12:26:45Z","abstract_excerpt":"In this paper we consider the frame-like formulation for the so called infinite (continuous) spin representations of the Poincare algebra. In the three dimensional case we give explicit Lagrangian formulation for bosonic and fermionic infinite spin fields (including the complete sets of the gauge invariant objects and all the necessary extra fields). Moreover we find the supertransformations for the supermultiplet containing one bosonic and one fermionic fields leaving the sum of their Lagrangians invariant. Properties of such fields and supermultiplets in four and higher dimensions are also b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.08832","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":""},"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":"2026-05-18T00:30:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcD0DARrynEVy6hfjhB+TyKT8HEqRWOsxusC/KCWKf7L+AeVHv27fLS+hUD2vtrhMPJ5IXZqMJg8i8gXW5SOAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:30:54.416176Z"},"content_sha256":"56c88fefa40739f0a7abdfd373530c658624339bc98e0f04557569e7933a9810","schema_version":"1.0","event_id":"sha256:56c88fefa40739f0a7abdfd373530c658624339bc98e0f04557569e7933a9810"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/bundle.json","state_url":"https://pith.science/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/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":"2026-05-27T15:30:54Z","links":{"resolver":"https://pith.science/pith/AIZPN6XEFO3KFRNQE3C5AZIP66","bundle":"https://pith.science/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/bundle.json","state":"https://pith.science/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AIZPN6XEFO3KFRNQE3C5AZIP66/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:AIZPN6XEFO3KFRNQE3C5AZIP66","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":"a68fdd479220a94f133da3299be674e9285766a495d21367029c040bbcbe9ea7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-27T12:26:45Z","title_canon_sha256":"8fcc8fba1031f6f789e8283da358f943d56fa8c88c156b5c8560e2b612a5ee96"},"schema_version":"1.0","source":{"id":"1707.08832","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.08832","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"arxiv_version","alias_value":"1707.08832v1","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.08832","created_at":"2026-05-18T00:30:30Z"},{"alias_kind":"pith_short_12","alias_value":"AIZPN6XEFO3K","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AIZPN6XEFO3KFRNQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AIZPN6XE","created_at":"2026-05-18T12:31:05Z"}],"graph_snapshots":[{"event_id":"sha256:56c88fefa40739f0a7abdfd373530c658624339bc98e0f04557569e7933a9810","target":"graph","created_at":"2026-05-18T00:30:30Z","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":"In this paper we consider the frame-like formulation for the so called infinite (continuous) spin representations of the Poincare algebra. In the three dimensional case we give explicit Lagrangian formulation for bosonic and fermionic infinite spin fields (including the complete sets of the gauge invariant objects and all the necessary extra fields). Moreover we find the supertransformations for the supermultiplet containing one bosonic and one fermionic fields leaving the sum of their Lagrangians invariant. Properties of such fields and supermultiplets in four and higher dimensions are also b","authors_text":"Yu. M. Zinoviev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-27T12:26:45Z","title":"Infinite spin fields in d = 3 and beyond"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.08832","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":"sha256:046dd3e0380c02ddc7ecb9df18ffaaf7a6966370b2c655cedb10657d68996540","target":"record","created_at":"2026-05-18T00:30:30Z","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":"a68fdd479220a94f133da3299be674e9285766a495d21367029c040bbcbe9ea7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-07-27T12:26:45Z","title_canon_sha256":"8fcc8fba1031f6f789e8283da358f943d56fa8c88c156b5c8560e2b612a5ee96"},"schema_version":"1.0","source":{"id":"1707.08832","kind":"arxiv","version":1}},"canonical_sha256":"0232f6fae42bb6a2c5b026c5d0650ff790aee142315679fdb5f5cb2f9e2c95ea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0232f6fae42bb6a2c5b026c5d0650ff790aee142315679fdb5f5cb2f9e2c95ea","first_computed_at":"2026-05-18T00:30:30.205299Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:30:30.205299Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a8GKVXOmEiiJpzcRhrUNGyunqidI8yq/Se8sJ39oyrbuYiKfweOE2uahZAnmIEzUU6JPaK3BR/aGkC/Rt1kpCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:30:30.205893Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.08832","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:046dd3e0380c02ddc7ecb9df18ffaaf7a6966370b2c655cedb10657d68996540","sha256:56c88fefa40739f0a7abdfd373530c658624339bc98e0f04557569e7933a9810"],"state_sha256":"f013b0302f14e31a38d9abf990fddde44a77277b512d86fbde29b043d035ae8e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X1f21YsByAiS2i0vfFhW0bm/d3Yhck75ns7WP/7v9HFnUPypburCZ/lp/IQRflWiB1Ci7OeDBNFwtUKmFKt0AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T15:30:54.419625Z","bundle_sha256":"54e3a024aa9ec05618ee82a181fe4675f45e55f5c4c7d296ae123d98d89094bd"}}