{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:ZNLMNZUE3RA2V6YNLGRUSCHMDM","short_pith_number":"pith:ZNLMNZUE","schema_version":"1.0","canonical_sha256":"cb56c6e684dc41aafb0d59a34908ec1b1cd8f18a4ebc59e48987f8f6f7201b48","source":{"kind":"arxiv","id":"2106.02166","version":2},"attestation_state":"computed","paper":{"title":"Gravitational Decoupling algorithm modifies the value of the conserved charges and thermodynamics properties in Lovelock Unique Vacuum theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Milko Estrada","submitted_at":"2021-06-03T22:42:12Z","abstract_excerpt":"We provide an extension of the Gravitational Decoupling (algorithm) for the Lovelock theory with Unique Vacuum (LUV), which represents a simple way to solve the equations of motion. Due to the application of this algorithm, the energy of the system splits in the {\\it energy of the seed solution} and the {\\it energy of each quasi-LUV sector}. Under certain assumptions imposed, the total energy varies due to the contribution of energy of each quasi-LUV sector. It is provided a new solution, whose energy differs from the energy of the seed solution in a quantity that depends on the number of extr"},"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":"2106.02166","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2021-06-03T22:42:12Z","cross_cats_sorted":[],"title_canon_sha256":"eedbb8bb4c39e625125f471b5ba1c859c8153805d65c376fb80a03e2b0fae5a5","abstract_canon_sha256":"f41174cc37a66e9c01bb6f48d6ab8dd1bf48d747db69fa6786b3940f2c82f495"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:56:46.979748Z","signature_b64":"HXXUCKaCqM7ECSzG6/d5ilXAtuql6Vxx3f2PzxnSarvXC3ovxzSm68l8KHdUZ2QL6+SK3twh7+de2DW30WKiCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb56c6e684dc41aafb0d59a34908ec1b1cd8f18a4ebc59e48987f8f6f7201b48","last_reissued_at":"2026-07-05T03:56:46.979284Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:56:46.979284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational Decoupling algorithm modifies the value of the conserved charges and thermodynamics properties in Lovelock Unique Vacuum theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Milko Estrada","submitted_at":"2021-06-03T22:42:12Z","abstract_excerpt":"We provide an extension of the Gravitational Decoupling (algorithm) for the Lovelock theory with Unique Vacuum (LUV), which represents a simple way to solve the equations of motion. Due to the application of this algorithm, the energy of the system splits in the {\\it energy of the seed solution} and the {\\it energy of each quasi-LUV sector}. Under certain assumptions imposed, the total energy varies due to the contribution of energy of each quasi-LUV sector. It is provided a new solution, whose energy differs from the energy of the seed solution in a quantity that depends on the number of extr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.02166","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.02166/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2106.02166","created_at":"2026-07-05T03:56:46.979339+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.02166v2","created_at":"2026-07-05T03:56:46.979339+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.02166","created_at":"2026-07-05T03:56:46.979339+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZNLMNZUE3RA2","created_at":"2026-07-05T03:56:46.979339+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZNLMNZUE3RA2V6YN","created_at":"2026-07-05T03:56:46.979339+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZNLMNZUE","created_at":"2026-07-05T03:56:46.979339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.01862","citing_title":"On static and rotating decoupled black holes without inner horizons","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM","json":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM.json","graph_json":"https://pith.science/api/pith-number/ZNLMNZUE3RA2V6YNLGRUSCHMDM/graph.json","events_json":"https://pith.science/api/pith-number/ZNLMNZUE3RA2V6YNLGRUSCHMDM/events.json","paper":"https://pith.science/paper/ZNLMNZUE"},"agent_actions":{"view_html":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM","download_json":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM.json","view_paper":"https://pith.science/paper/ZNLMNZUE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.02166&json=true","fetch_graph":"https://pith.science/api/pith-number/ZNLMNZUE3RA2V6YNLGRUSCHMDM/graph.json","fetch_events":"https://pith.science/api/pith-number/ZNLMNZUE3RA2V6YNLGRUSCHMDM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM/action/storage_attestation","attest_author":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM/action/author_attestation","sign_citation":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM/action/citation_signature","submit_replication":"https://pith.science/pith/ZNLMNZUE3RA2V6YNLGRUSCHMDM/action/replication_record"}},"created_at":"2026-07-05T03:56:46.979339+00:00","updated_at":"2026-07-05T03:56:46.979339+00:00"}