{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:HBCLBGYME6XVS7OSO767U2NVM6","short_pith_number":"pith:HBCLBGYM","canonical_record":{"source":{"id":"0709.4392","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2007-09-27T13:42:14Z","cross_cats_sorted":[],"title_canon_sha256":"02dcc8649c470e8c12b942acbe59d1dfaa1690ac248e2eb7ac78a1b923ea97c0","abstract_canon_sha256":"771f3141d3cd4738f87d0a3635d1aaa6277e0a7dad441749dda567098ca6049f"},"schema_version":"1.0"},"canonical_sha256":"3844b09b0c27af597dd277fdfa69b56781f6bd97c729d75620037a804fd53f97","source":{"kind":"arxiv","id":"0709.4392","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0709.4392","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"arxiv_version","alias_value":"0709.4392v2","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0709.4392","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"pith_short_12","alias_value":"HBCLBGYME6XV","created_at":"2026-05-18T12:25:55Z"},{"alias_kind":"pith_short_16","alias_value":"HBCLBGYME6XVS7OS","created_at":"2026-05-18T12:25:55Z"},{"alias_kind":"pith_short_8","alias_value":"HBCLBGYM","created_at":"2026-05-18T12:25:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:HBCLBGYME6XVS7OSO767U2NVM6","target":"record","payload":{"canonical_record":{"source":{"id":"0709.4392","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2007-09-27T13:42:14Z","cross_cats_sorted":[],"title_canon_sha256":"02dcc8649c470e8c12b942acbe59d1dfaa1690ac248e2eb7ac78a1b923ea97c0","abstract_canon_sha256":"771f3141d3cd4738f87d0a3635d1aaa6277e0a7dad441749dda567098ca6049f"},"schema_version":"1.0"},"canonical_sha256":"3844b09b0c27af597dd277fdfa69b56781f6bd97c729d75620037a804fd53f97","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:16:10.896415Z","signature_b64":"oxFfVWE8nj/I5zz1pHyVsvC0M32SWsjEItZD2xzq/fcMLGuSuffb6WjcE6dk1jYtHhoy1RzI8wOiSPv+ws8cCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3844b09b0c27af597dd277fdfa69b56781f6bd97c729d75620037a804fd53f97","last_reissued_at":"2026-05-18T02:16:10.895869Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:16:10.895869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0709.4392","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":"2026-05-18T02:16:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Vqh/NaaZfBrldf4SR/KZPeeaBAk3O1DGXi9JkV4PB0GrApjY+CUw89c3epHjDdzpCcYTLEqH8zYwKt3p9wQiAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T20:38:51.170189Z"},"content_sha256":"3449d9f0f436f1fc45e99934cc7c67693911ce4c0553550175af3dc2bd032aa1","schema_version":"1.0","event_id":"sha256:3449d9f0f436f1fc45e99934cc7c67693911ce4c0553550175af3dc2bd032aa1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:HBCLBGYME6XVS7OSO767U2NVM6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ordinary-derivative formulation of conformal totally symmetric arbitrary spin bosonic fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R. R. Metsaev","submitted_at":"2007-09-27T13:42:14Z","abstract_excerpt":"Conformal totally symmetric arbitrary spin bosonic fields in flat space-time of even dimension greater than or equal to four are studied. Second-derivative (ordinary-derivative) formulation for such fields is developed. We obtain gauge invariant Lagrangian and the corresponding gauge transformations. Gauge symmetries are realized by involving the Stueckelberg and auxiliary fields. Realization of global conformal boost symmetries on conformal gauge fields is obtained. Modified de Donder gauge condition and de Donder-Stueckelberg gauge condition are introduced. Using the de Donder-Stueckelberg g"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0709.4392","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":"2026-05-18T02:16:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mx+2fzIFV/TI6YTLtYFWZB6xAv+ddk8w3yA8zf/t9yG+4edygXmAfX+6YRvl1Hs4oFBr0tO4nr4uvkawdzfeBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T20:38:51.170869Z"},"content_sha256":"a7025113e012608abb9e2d59ba23d8a4dfbf6dfe715ec49f174e1f9d8dbc3135","schema_version":"1.0","event_id":"sha256:a7025113e012608abb9e2d59ba23d8a4dfbf6dfe715ec49f174e1f9d8dbc3135"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HBCLBGYME6XVS7OSO767U2NVM6/bundle.json","state_url":"https://pith.science/pith/HBCLBGYME6XVS7OSO767U2NVM6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HBCLBGYME6XVS7OSO767U2NVM6/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":"2026-05-25T20:38:51Z","links":{"resolver":"https://pith.science/pith/HBCLBGYME6XVS7OSO767U2NVM6","bundle":"https://pith.science/pith/HBCLBGYME6XVS7OSO767U2NVM6/bundle.json","state":"https://pith.science/pith/HBCLBGYME6XVS7OSO767U2NVM6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HBCLBGYME6XVS7OSO767U2NVM6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:HBCLBGYME6XVS7OSO767U2NVM6","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":"771f3141d3cd4738f87d0a3635d1aaa6277e0a7dad441749dda567098ca6049f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2007-09-27T13:42:14Z","title_canon_sha256":"02dcc8649c470e8c12b942acbe59d1dfaa1690ac248e2eb7ac78a1b923ea97c0"},"schema_version":"1.0","source":{"id":"0709.4392","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0709.4392","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"arxiv_version","alias_value":"0709.4392v2","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0709.4392","created_at":"2026-05-18T02:16:10Z"},{"alias_kind":"pith_short_12","alias_value":"HBCLBGYME6XV","created_at":"2026-05-18T12:25:55Z"},{"alias_kind":"pith_short_16","alias_value":"HBCLBGYME6XVS7OS","created_at":"2026-05-18T12:25:55Z"},{"alias_kind":"pith_short_8","alias_value":"HBCLBGYM","created_at":"2026-05-18T12:25:55Z"}],"graph_snapshots":[{"event_id":"sha256:a7025113e012608abb9e2d59ba23d8a4dfbf6dfe715ec49f174e1f9d8dbc3135","target":"graph","created_at":"2026-05-18T02:16:10Z","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":"Conformal totally symmetric arbitrary spin bosonic fields in flat space-time of even dimension greater than or equal to four are studied. Second-derivative (ordinary-derivative) formulation for such fields is developed. We obtain gauge invariant Lagrangian and the corresponding gauge transformations. Gauge symmetries are realized by involving the Stueckelberg and auxiliary fields. Realization of global conformal boost symmetries on conformal gauge fields is obtained. Modified de Donder gauge condition and de Donder-Stueckelberg gauge condition are introduced. Using the de Donder-Stueckelberg g","authors_text":"R. R. Metsaev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2007-09-27T13:42:14Z","title":"Ordinary-derivative formulation of conformal totally symmetric arbitrary spin bosonic fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0709.4392","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":"sha256:3449d9f0f436f1fc45e99934cc7c67693911ce4c0553550175af3dc2bd032aa1","target":"record","created_at":"2026-05-18T02:16:10Z","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":"771f3141d3cd4738f87d0a3635d1aaa6277e0a7dad441749dda567098ca6049f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2007-09-27T13:42:14Z","title_canon_sha256":"02dcc8649c470e8c12b942acbe59d1dfaa1690ac248e2eb7ac78a1b923ea97c0"},"schema_version":"1.0","source":{"id":"0709.4392","kind":"arxiv","version":2}},"canonical_sha256":"3844b09b0c27af597dd277fdfa69b56781f6bd97c729d75620037a804fd53f97","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3844b09b0c27af597dd277fdfa69b56781f6bd97c729d75620037a804fd53f97","first_computed_at":"2026-05-18T02:16:10.895869Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:16:10.895869Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oxFfVWE8nj/I5zz1pHyVsvC0M32SWsjEItZD2xzq/fcMLGuSuffb6WjcE6dk1jYtHhoy1RzI8wOiSPv+ws8cCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:16:10.896415Z","signed_message":"canonical_sha256_bytes"},"source_id":"0709.4392","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3449d9f0f436f1fc45e99934cc7c67693911ce4c0553550175af3dc2bd032aa1","sha256:a7025113e012608abb9e2d59ba23d8a4dfbf6dfe715ec49f174e1f9d8dbc3135"],"state_sha256":"2554ae1556f48441ca150d5ae8a534be06cf9056f0accaeaf3fe871fd467dd31"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kJgJDHkkJkOBWHZyIhNiIy4rKli9U/W0n6apm1M3POk/nuk50ygwWCUtzhvWk0mI+fw14NVm6WECh2mhJwLOAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T20:38:51.174301Z","bundle_sha256":"235e747bee109ac9e4dbcee9bc2a1f57ec963165547623e8b27d87dfed4c2aed"}}