{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:T2LOCVM5ZBAKS4BC4L5VHRZI3E","short_pith_number":"pith:T2LOCVM5","schema_version":"1.0","canonical_sha256":"9e96e1559dc840a97022e2fb53c728d91ae7103f5be09fa0aba160dedc4e496b","source":{"kind":"arxiv","id":"1001.3407","version":2},"attestation_state":"computed","paper":{"title":"Consistent Gravitationally-Coupled Spin-2 Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"H. I. Arcos, J. G. Pereira, Tiago Gribl Lucas","submitted_at":"2010-01-19T21:00:21Z","abstract_excerpt":"Inspired by the translational gauge structure of teleparallel gravity, the theory for a fundamental massless spin-2 field is constructed. Accordingly, instead of being represented by a symmetric second-rank tensor, the fundamental spin-2 field is assumed to be represented by a spacetime (world) vector field assuming values in the Lie algebra of the translation group. The flat-space theory naturally emerges in the Fierz formalism and is found to be equivalent to the usual metric-based theory. However, the gravitationally coupled theory, with gravitation itself described by teleparallel gravity,"},"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":"1001.3407","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-01-19T21:00:21Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"33224de08e68357fba62a414ec8ba97dbbd8e7cf23bf8ac9096efd20771afb5c","abstract_canon_sha256":"9b909a925a8dbdaa5dfa18b746b5ec126516cb566173d749063f9a911a8b4bc7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:32:28.841835Z","signature_b64":"ZcB3h5K56w3x9MeMaHhRdgNISjMwtJ2JIhbB3RiMyNtj6qi9kNA0AJc9qJ1C9mryGrU6HnhZVNKVxU+2nnUkBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e96e1559dc840a97022e2fb53c728d91ae7103f5be09fa0aba160dedc4e496b","last_reissued_at":"2026-05-18T03:32:28.841284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:32:28.841284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Consistent Gravitationally-Coupled Spin-2 Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"H. I. Arcos, J. G. Pereira, Tiago Gribl Lucas","submitted_at":"2010-01-19T21:00:21Z","abstract_excerpt":"Inspired by the translational gauge structure of teleparallel gravity, the theory for a fundamental massless spin-2 field is constructed. Accordingly, instead of being represented by a symmetric second-rank tensor, the fundamental spin-2 field is assumed to be represented by a spacetime (world) vector field assuming values in the Lie algebra of the translation group. The flat-space theory naturally emerges in the Fierz formalism and is found to be equivalent to the usual metric-based theory. However, the gravitationally coupled theory, with gravitation itself described by teleparallel gravity,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.3407","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1001.3407","created_at":"2026-05-18T03:32:28.841388+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.3407v2","created_at":"2026-05-18T03:32:28.841388+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.3407","created_at":"2026-05-18T03:32:28.841388+00:00"},{"alias_kind":"pith_short_12","alias_value":"T2LOCVM5ZBAK","created_at":"2026-05-18T12:26:13.927090+00:00"},{"alias_kind":"pith_short_16","alias_value":"T2LOCVM5ZBAKS4BC","created_at":"2026-05-18T12:26:13.927090+00:00"},{"alias_kind":"pith_short_8","alias_value":"T2LOCVM5","created_at":"2026-05-18T12:26:13.927090+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/T2LOCVM5ZBAKS4BC4L5VHRZI3E","json":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E.json","graph_json":"https://pith.science/api/pith-number/T2LOCVM5ZBAKS4BC4L5VHRZI3E/graph.json","events_json":"https://pith.science/api/pith-number/T2LOCVM5ZBAKS4BC4L5VHRZI3E/events.json","paper":"https://pith.science/paper/T2LOCVM5"},"agent_actions":{"view_html":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E","download_json":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E.json","view_paper":"https://pith.science/paper/T2LOCVM5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.3407&json=true","fetch_graph":"https://pith.science/api/pith-number/T2LOCVM5ZBAKS4BC4L5VHRZI3E/graph.json","fetch_events":"https://pith.science/api/pith-number/T2LOCVM5ZBAKS4BC4L5VHRZI3E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E/action/storage_attestation","attest_author":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E/action/author_attestation","sign_citation":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E/action/citation_signature","submit_replication":"https://pith.science/pith/T2LOCVM5ZBAKS4BC4L5VHRZI3E/action/replication_record"}},"created_at":"2026-05-18T03:32:28.841388+00:00","updated_at":"2026-05-18T03:32:28.841388+00:00"}