{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:PLJ6PJMOFQIWLBTVELOZMRKXSQ","short_pith_number":"pith:PLJ6PJMO","schema_version":"1.0","canonical_sha256":"7ad3e7a58e2c1165867522dd9645579439564bdb4e9b38d7cb89ba03589c6216","source":{"kind":"arxiv","id":"1109.1382","version":1},"attestation_state":"computed","paper":{"title":"Graviton in a Curved Space-Time Background and Gauge Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","math.MP"],"primary_cat":"math-ph","authors_text":"N.G. Tokarevskaya, V.M. Red'kov, V.V. Kisel","submitted_at":"2011-09-07T08:09:07Z","abstract_excerpt":"Pauli-Fierz approach to description of a massless spin-2 particle is investigated in the framework of 30-component first order relativistic wave equation theory on a curved space-time background. It is shown that additional gauge symmetry of massless equations established by Pauli-Fierz can be extended only to curved space-time regions where Ricci tensor vanishes. In all such space-time models the generally covariant S=2 massless wave equation exhibits gauge symmetry property, otherwise it is not so."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1109.1382","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2011-09-07T08:09:07Z","cross_cats_sorted":["gr-qc","math.MP"],"title_canon_sha256":"b28c55374ab01ffab2bc986f22b56ed8a4664aa17a475a6035aec9969a44acc0","abstract_canon_sha256":"f2599ae16ad07fce44fd1a196e6186bb68b518dd557c63880e2de8bdfbc8fc58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:55.812704Z","signature_b64":"3ytS/6mbQq5Co3w26hh5PHCKZUIdfEIcYy5gV64h4S8Chrt8Z+ofXwmaA5zZSp6sd/x8ArbAHRa8IrDQOiCHAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ad3e7a58e2c1165867522dd9645579439564bdb4e9b38d7cb89ba03589c6216","last_reissued_at":"2026-05-18T04:13:55.812196Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:55.812196Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Graviton in a Curved Space-Time Background and Gauge Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","math.MP"],"primary_cat":"math-ph","authors_text":"N.G. Tokarevskaya, V.M. Red'kov, V.V. Kisel","submitted_at":"2011-09-07T08:09:07Z","abstract_excerpt":"Pauli-Fierz approach to description of a massless spin-2 particle is investigated in the framework of 30-component first order relativistic wave equation theory on a curved space-time background. It is shown that additional gauge symmetry of massless equations established by Pauli-Fierz can be extended only to curved space-time regions where Ricci tensor vanishes. In all such space-time models the generally covariant S=2 massless wave equation exhibits gauge symmetry property, otherwise it is not so."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.1382","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1109.1382","created_at":"2026-05-18T04:13:55.812268+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.1382v1","created_at":"2026-05-18T04:13:55.812268+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.1382","created_at":"2026-05-18T04:13:55.812268+00:00"},{"alias_kind":"pith_short_12","alias_value":"PLJ6PJMOFQIW","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"PLJ6PJMOFQIWLBTV","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"PLJ6PJMO","created_at":"2026-05-18T12:26:39.201973+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ","json":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ.json","graph_json":"https://pith.science/api/pith-number/PLJ6PJMOFQIWLBTVELOZMRKXSQ/graph.json","events_json":"https://pith.science/api/pith-number/PLJ6PJMOFQIWLBTVELOZMRKXSQ/events.json","paper":"https://pith.science/paper/PLJ6PJMO"},"agent_actions":{"view_html":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ","download_json":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ.json","view_paper":"https://pith.science/paper/PLJ6PJMO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.1382&json=true","fetch_graph":"https://pith.science/api/pith-number/PLJ6PJMOFQIWLBTVELOZMRKXSQ/graph.json","fetch_events":"https://pith.science/api/pith-number/PLJ6PJMOFQIWLBTVELOZMRKXSQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ/action/storage_attestation","attest_author":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ/action/author_attestation","sign_citation":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ/action/citation_signature","submit_replication":"https://pith.science/pith/PLJ6PJMOFQIWLBTVELOZMRKXSQ/action/replication_record"}},"created_at":"2026-05-18T04:13:55.812268+00:00","updated_at":"2026-05-18T04:13:55.812268+00:00"}