{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:PK3ULZ2XOLHASII3DY4UAW5ZKP","short_pith_number":"pith:PK3ULZ2X","schema_version":"1.0","canonical_sha256":"7ab745e75772ce09211b1e39405bb953f8f6d92a13901c0b4f4137856f28477d","source":{"kind":"arxiv","id":"1504.07657","version":2},"attestation_state":"computed","paper":{"title":"Dilatonic dyon black hole solutions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"K.A. Boshkayev, M.E. Abishev, V.D. Dzhunushaliev, V.D. Ivashchuk","submitted_at":"2015-04-28T20:58:39Z","abstract_excerpt":"Dilatonic black hole dyon solutions with arbitrary dilatonic coupling constant $\\lambda \\neq 0$ and canonical sign $\\varepsilon = +1$ for scalar field kynetic term are considered. These solutions are defined up to solutions of two master equations for moduli funtions. For $\\lambda^2 \\neq 1/2$ the solutions are extended to $\\varepsilon = \\pm 1$, where $\\varepsilon = -1$ corresponds to ghost (phantom) scalar field. Some physical parameters of the solutions: gravitational mass, scalar charge, Hawking temperature, black hole area entropy and parametrized post-Newtonian (PPN) parameters $\\beta$ and"},"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":"1504.07657","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T20:58:39Z","cross_cats_sorted":[],"title_canon_sha256":"db5b48f6964d3898e41a62bb1d608a05391249af91737085c4864e774534403f","abstract_canon_sha256":"2fde2137790f911b586a2b7c3d5d25efdda56fec3b16338c5bf30041d219f304"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:24.773828Z","signature_b64":"rYBWYf+rpMG59Mo0W9/VrezHDwGOVdjcZoF3UKz7a1cIJFhVsYKpYKXtJ4WnJlbrwI5Pj66YqZnAt5dLf6B5Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ab745e75772ce09211b1e39405bb953f8f6d92a13901c0b4f4137856f28477d","last_reissued_at":"2026-05-18T01:51:24.773159Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:24.773159Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dilatonic dyon black hole solutions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"K.A. Boshkayev, M.E. Abishev, V.D. Dzhunushaliev, V.D. Ivashchuk","submitted_at":"2015-04-28T20:58:39Z","abstract_excerpt":"Dilatonic black hole dyon solutions with arbitrary dilatonic coupling constant $\\lambda \\neq 0$ and canonical sign $\\varepsilon = +1$ for scalar field kynetic term are considered. These solutions are defined up to solutions of two master equations for moduli funtions. For $\\lambda^2 \\neq 1/2$ the solutions are extended to $\\varepsilon = \\pm 1$, where $\\varepsilon = -1$ corresponds to ghost (phantom) scalar field. Some physical parameters of the solutions: gravitational mass, scalar charge, Hawking temperature, black hole area entropy and parametrized post-Newtonian (PPN) parameters $\\beta$ and"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.07657","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":"1504.07657","created_at":"2026-05-18T01:51:24.773267+00:00"},{"alias_kind":"arxiv_version","alias_value":"1504.07657v2","created_at":"2026-05-18T01:51:24.773267+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.07657","created_at":"2026-05-18T01:51:24.773267+00:00"},{"alias_kind":"pith_short_12","alias_value":"PK3ULZ2XOLHA","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"PK3ULZ2XOLHASII3","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"PK3ULZ2X","created_at":"2026-05-18T12:29:37.295048+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/PK3ULZ2XOLHASII3DY4UAW5ZKP","json":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP.json","graph_json":"https://pith.science/api/pith-number/PK3ULZ2XOLHASII3DY4UAW5ZKP/graph.json","events_json":"https://pith.science/api/pith-number/PK3ULZ2XOLHASII3DY4UAW5ZKP/events.json","paper":"https://pith.science/paper/PK3ULZ2X"},"agent_actions":{"view_html":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP","download_json":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP.json","view_paper":"https://pith.science/paper/PK3ULZ2X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1504.07657&json=true","fetch_graph":"https://pith.science/api/pith-number/PK3ULZ2XOLHASII3DY4UAW5ZKP/graph.json","fetch_events":"https://pith.science/api/pith-number/PK3ULZ2XOLHASII3DY4UAW5ZKP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP/action/storage_attestation","attest_author":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP/action/author_attestation","sign_citation":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP/action/citation_signature","submit_replication":"https://pith.science/pith/PK3ULZ2XOLHASII3DY4UAW5ZKP/action/replication_record"}},"created_at":"2026-05-18T01:51:24.773267+00:00","updated_at":"2026-05-18T01:51:24.773267+00:00"}