{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:QTJYNJKSTE55WAXU5TXWQBKPLL","short_pith_number":"pith:QTJYNJKS","schema_version":"1.0","canonical_sha256":"84d386a552993bdb02f4ecef68054f5ada7634b68862b9a8a683cfe7af5904a2","source":{"kind":"arxiv","id":"1701.02029","version":3},"attestation_state":"computed","paper":{"title":"Dilatonic dyon-like black hole solutions in the model with two Abelian gauge fields","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. Ivashchuk","submitted_at":"2017-01-08T22:32:31Z","abstract_excerpt":"Dilatonic black hole dyon-like solutions in the gravitational $4d$ model with a scalar field, two 2-forms, two dilatonic coupling constants $\\lambda_i \\neq 0$, $i =1,2$, obeying $\\lambda_1 \\neq - \\lambda_2$ and the sign parameter $\\varepsilon = \\pm 1$ for scalar field kinetic term are considered. Here $\\varepsilon = - 1$ corresponds to a ghost scalar field. These solutions are defined up to solutions of two master equations for two moduli functions, when $\\lambda^2_i \\neq 1/2$ for $\\varepsilon = - 1$. Some physical parameters of the solutions are obtained: gravitational mass, scalar charge, Ha"},"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":"1701.02029","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-01-08T22:32:31Z","cross_cats_sorted":[],"title_canon_sha256":"7e017fc76235a1b139feb805e6422db4ba3d63b785794c3516781cfbb8d648e7","abstract_canon_sha256":"7b8c563475ed98ffa1763dc78f94325e4dd9c471f0629aa797557746762df116"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:43.169089Z","signature_b64":"QUlYKDq4UuYq6ti/zNO8VnqAX8eCNvln+Kw21CC6wM17sCcnaD+mtxW5tAWeBCvgqNRc3pDxp3rdV6mou9QJCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84d386a552993bdb02f4ecef68054f5ada7634b68862b9a8a683cfe7af5904a2","last_reissued_at":"2026-05-18T00:45:43.168425Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:43.168425Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dilatonic dyon-like black hole solutions in the model with two Abelian gauge fields","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. Ivashchuk","submitted_at":"2017-01-08T22:32:31Z","abstract_excerpt":"Dilatonic black hole dyon-like solutions in the gravitational $4d$ model with a scalar field, two 2-forms, two dilatonic coupling constants $\\lambda_i \\neq 0$, $i =1,2$, obeying $\\lambda_1 \\neq - \\lambda_2$ and the sign parameter $\\varepsilon = \\pm 1$ for scalar field kinetic term are considered. Here $\\varepsilon = - 1$ corresponds to a ghost scalar field. These solutions are defined up to solutions of two master equations for two moduli functions, when $\\lambda^2_i \\neq 1/2$ for $\\varepsilon = - 1$. Some physical parameters of the solutions are obtained: gravitational mass, scalar charge, Ha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.02029","kind":"arxiv","version":3},"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":"1701.02029","created_at":"2026-05-18T00:45:43.168536+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.02029v3","created_at":"2026-05-18T00:45:43.168536+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.02029","created_at":"2026-05-18T00:45:43.168536+00:00"},{"alias_kind":"pith_short_12","alias_value":"QTJYNJKSTE55","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"QTJYNJKSTE55WAXU","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"QTJYNJKS","created_at":"2026-05-18T12:31:39.905425+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/QTJYNJKSTE55WAXU5TXWQBKPLL","json":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL.json","graph_json":"https://pith.science/api/pith-number/QTJYNJKSTE55WAXU5TXWQBKPLL/graph.json","events_json":"https://pith.science/api/pith-number/QTJYNJKSTE55WAXU5TXWQBKPLL/events.json","paper":"https://pith.science/paper/QTJYNJKS"},"agent_actions":{"view_html":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL","download_json":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL.json","view_paper":"https://pith.science/paper/QTJYNJKS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.02029&json=true","fetch_graph":"https://pith.science/api/pith-number/QTJYNJKSTE55WAXU5TXWQBKPLL/graph.json","fetch_events":"https://pith.science/api/pith-number/QTJYNJKSTE55WAXU5TXWQBKPLL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL/action/storage_attestation","attest_author":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL/action/author_attestation","sign_citation":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL/action/citation_signature","submit_replication":"https://pith.science/pith/QTJYNJKSTE55WAXU5TXWQBKPLL/action/replication_record"}},"created_at":"2026-05-18T00:45:43.168536+00:00","updated_at":"2026-05-18T00:45:43.168536+00:00"}