{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:TW4RYZ4GBZMD2JTOIQACUUVUYQ","short_pith_number":"pith:TW4RYZ4G","schema_version":"1.0","canonical_sha256":"9db91c67860e583d266e44002a52b4c435dd27380b8d0dffdc8684e75b90ccfe","source":{"kind":"arxiv","id":"1708.04947","version":2},"attestation_state":"computed","paper":{"title":"Non-singular spacetimes with a negative cosmological constant: IV. Stationary black hole solutions with matter fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math.DG"],"primary_cat":"gr-qc","authors_text":"Erwann Delay, Paul Klinger, Piotr T. Chru\\'sciel","submitted_at":"2017-08-16T15:42:49Z","abstract_excerpt":"We use an elliptic system of equations with complex coefficients for a set of complex-valued tensor fields as a tool to construct infinite-dimensional families of non-singular stationary black holes, real-valued Lorentzian solutions of the Einstein-Maxwell-dilaton-scalar fields-Yang-Mills-Higgs-Chern-Simons-$f(R)$ equations with a negative cosmological constant. The families include an infinite-dimensional family of solutions with the usual AdS conformal structure at conformal infinity."},"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":"1708.04947","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-16T15:42:49Z","cross_cats_sorted":["hep-th","math.DG"],"title_canon_sha256":"f9b57abb12009a857720ca0cb4b0b64407b3c4db105ab22d307bccc784cd0bfd","abstract_canon_sha256":"2f6c083afbd075b3b8a71a87b42eb6a5221c46ad4fcae2a4c6d646511a9453b4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:14.682862Z","signature_b64":"F+S+6p3TQo8U0O+vw4NQ2cBLu422NnpvELcKZ48CvlLf5t7OPmjH0V0KMwSmmoUtpdqHKtJs6W/KXjNPadW1BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9db91c67860e583d266e44002a52b4c435dd27380b8d0dffdc8684e75b90ccfe","last_reissued_at":"2026-05-18T00:28:14.682204Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:14.682204Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-singular spacetimes with a negative cosmological constant: IV. Stationary black hole solutions with matter fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math.DG"],"primary_cat":"gr-qc","authors_text":"Erwann Delay, Paul Klinger, Piotr T. Chru\\'sciel","submitted_at":"2017-08-16T15:42:49Z","abstract_excerpt":"We use an elliptic system of equations with complex coefficients for a set of complex-valued tensor fields as a tool to construct infinite-dimensional families of non-singular stationary black holes, real-valued Lorentzian solutions of the Einstein-Maxwell-dilaton-scalar fields-Yang-Mills-Higgs-Chern-Simons-$f(R)$ equations with a negative cosmological constant. The families include an infinite-dimensional family of solutions with the usual AdS conformal structure at conformal infinity."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.04947","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":"1708.04947","created_at":"2026-05-18T00:28:14.682291+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.04947v2","created_at":"2026-05-18T00:28:14.682291+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.04947","created_at":"2026-05-18T00:28:14.682291+00:00"},{"alias_kind":"pith_short_12","alias_value":"TW4RYZ4GBZMD","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"TW4RYZ4GBZMD2JTO","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"TW4RYZ4G","created_at":"2026-05-18T12:31:46.661854+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.10877","citing_title":"Holographic is Hamiltonian, relatively","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ","json":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ.json","graph_json":"https://pith.science/api/pith-number/TW4RYZ4GBZMD2JTOIQACUUVUYQ/graph.json","events_json":"https://pith.science/api/pith-number/TW4RYZ4GBZMD2JTOIQACUUVUYQ/events.json","paper":"https://pith.science/paper/TW4RYZ4G"},"agent_actions":{"view_html":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ","download_json":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ.json","view_paper":"https://pith.science/paper/TW4RYZ4G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.04947&json=true","fetch_graph":"https://pith.science/api/pith-number/TW4RYZ4GBZMD2JTOIQACUUVUYQ/graph.json","fetch_events":"https://pith.science/api/pith-number/TW4RYZ4GBZMD2JTOIQACUUVUYQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ/action/storage_attestation","attest_author":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ/action/author_attestation","sign_citation":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ/action/citation_signature","submit_replication":"https://pith.science/pith/TW4RYZ4GBZMD2JTOIQACUUVUYQ/action/replication_record"}},"created_at":"2026-05-18T00:28:14.682291+00:00","updated_at":"2026-05-18T00:28:14.682291+00:00"}