{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YEZACSBORPHES7LIL3XSUEY2KH","short_pith_number":"pith:YEZACSBO","schema_version":"1.0","canonical_sha256":"c13201482e8bce497d685eef2a131a51e0458e7607013d63394e85d47f41a9f5","source":{"kind":"arxiv","id":"1503.04882","version":1},"attestation_state":"computed","paper":{"title":"A Rastall Scalar-Tensor theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"A.M. Oliveira, M.H. Daouda J.C. Fabris, O.F. Piattella, T. Caram\\^es, V. Strokov","submitted_at":"2015-03-17T00:20:25Z","abstract_excerpt":"We formulate a theory combining the principles of a scalar-tensor gravity and the Rastall proposal of a violation of the usual conservation laws. In the resulting Brans-Dicke-Rastall (BDR) theory the only exact, static, spherically symmetric solution is a Robinson-Bertotti type solution besides the trivial Schwarzschild one. The PPN constraints can be completely satisfied for some values of the free parameters.The cosmological solutions display, among others, a decelerate-accelerate transition in the matter dominated phase."},"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":"1503.04882","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-03-17T00:20:25Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"ab4342eb5492d87bb4bd58bf125bc773a4ad77df25d761b6965be2e961040050","abstract_canon_sha256":"52270fe8ce946f34ed91fddf1e89e3c06563ea06cd38419c8c7eed7f9c84f054"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:21.332968Z","signature_b64":"qMms2oWJ4XJy5tXevvJZgn3SM/6m98nJXEI3IRBh75rTAX6KnZcN+omHrt9bQAlffIazK2ShOjZwxr59aDmXCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c13201482e8bce497d685eef2a131a51e0458e7607013d63394e85d47f41a9f5","last_reissued_at":"2026-05-18T02:22:21.332234Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:21.332234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Rastall Scalar-Tensor theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"A.M. Oliveira, M.H. Daouda J.C. Fabris, O.F. Piattella, T. Caram\\^es, V. Strokov","submitted_at":"2015-03-17T00:20:25Z","abstract_excerpt":"We formulate a theory combining the principles of a scalar-tensor gravity and the Rastall proposal of a violation of the usual conservation laws. In the resulting Brans-Dicke-Rastall (BDR) theory the only exact, static, spherically symmetric solution is a Robinson-Bertotti type solution besides the trivial Schwarzschild one. The PPN constraints can be completely satisfied for some values of the free parameters.The cosmological solutions display, among others, a decelerate-accelerate transition in the matter dominated phase."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.04882","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":"1503.04882","created_at":"2026-05-18T02:22:21.332402+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.04882v1","created_at":"2026-05-18T02:22:21.332402+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.04882","created_at":"2026-05-18T02:22:21.332402+00:00"},{"alias_kind":"pith_short_12","alias_value":"YEZACSBORPHE","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"YEZACSBORPHES7LI","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"YEZACSBO","created_at":"2026-05-18T12:29:50.041715+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/YEZACSBORPHES7LIL3XSUEY2KH","json":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH.json","graph_json":"https://pith.science/api/pith-number/YEZACSBORPHES7LIL3XSUEY2KH/graph.json","events_json":"https://pith.science/api/pith-number/YEZACSBORPHES7LIL3XSUEY2KH/events.json","paper":"https://pith.science/paper/YEZACSBO"},"agent_actions":{"view_html":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH","download_json":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH.json","view_paper":"https://pith.science/paper/YEZACSBO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.04882&json=true","fetch_graph":"https://pith.science/api/pith-number/YEZACSBORPHES7LIL3XSUEY2KH/graph.json","fetch_events":"https://pith.science/api/pith-number/YEZACSBORPHES7LIL3XSUEY2KH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH/action/storage_attestation","attest_author":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH/action/author_attestation","sign_citation":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH/action/citation_signature","submit_replication":"https://pith.science/pith/YEZACSBORPHES7LIL3XSUEY2KH/action/replication_record"}},"created_at":"2026-05-18T02:22:21.332402+00:00","updated_at":"2026-05-18T02:22:21.332402+00:00"}