{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:7CWHD76RZMQ6B2A23H4VRDBB4I","short_pith_number":"pith:7CWHD76R","schema_version":"1.0","canonical_sha256":"f8ac71ffd1cb21e0e81ad9f9588c21e20ffd46fa997070a02fcf6d94364f734f","source":{"kind":"arxiv","id":"1304.5206","version":2},"attestation_state":"computed","paper":{"title":"A new Einstein-nonlinear electrodynamics solution in 2+1-dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Halilsoy, Ozay Gurtug, S. Habib Mazharimousavi","submitted_at":"2013-04-17T10:36:32Z","abstract_excerpt":"We introduce a class of solutions in $2+1-$dimensional Einstein-Power-Maxwell theory for circularly symmetric electric field. The electromagnetic field is considered with an angular component given by $% F_{\\mu \\nu }=E_{0}\\delta_{\\mu }^{t}\\delta_{\\nu }^{\\theta }$ for $E_{0}=$ constant. First, we show that the metric for zero cosmological constant and the Power-Maxwell Lagrangian of the form of $\\sqrt{\\left\\vert F_{\\mu \\nu }F^{\\mu \\nu }\\right\\vert }$, coincides with the solution given in $2+1-$% dimensional gravity coupled with a massless, self interacting real scalar field. With the same Lagra"},"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":"1304.5206","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-04-17T10:36:32Z","cross_cats_sorted":[],"title_canon_sha256":"bc525099d3eb6ad253e7d66c2313ee71fefc05f061537df5339c72569017ef49","abstract_canon_sha256":"5ad29d3e2b0ac2fb6110fc7fa550f6d4aa4fa289884d19e6bb144c5b27482894"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:39.536941Z","signature_b64":"XNO0haWakS9Im0dODP/mR0Rfw3eJ+PcgnweZQbTYAAm6SF/0R3WDbSrcvGDPV/YYbDda0Vs5Z1UhCO/Y6dwbDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8ac71ffd1cb21e0e81ad9f9588c21e20ffd46fa997070a02fcf6d94364f734f","last_reissued_at":"2026-05-18T03:00:39.536335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:39.536335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A new Einstein-nonlinear electrodynamics solution in 2+1-dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Halilsoy, Ozay Gurtug, S. Habib Mazharimousavi","submitted_at":"2013-04-17T10:36:32Z","abstract_excerpt":"We introduce a class of solutions in $2+1-$dimensional Einstein-Power-Maxwell theory for circularly symmetric electric field. The electromagnetic field is considered with an angular component given by $% F_{\\mu \\nu }=E_{0}\\delta_{\\mu }^{t}\\delta_{\\nu }^{\\theta }$ for $E_{0}=$ constant. First, we show that the metric for zero cosmological constant and the Power-Maxwell Lagrangian of the form of $\\sqrt{\\left\\vert F_{\\mu \\nu }F^{\\mu \\nu }\\right\\vert }$, coincides with the solution given in $2+1-$% dimensional gravity coupled with a massless, self interacting real scalar field. With the same Lagra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.5206","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":"1304.5206","created_at":"2026-05-18T03:00:39.536440+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.5206v2","created_at":"2026-05-18T03:00:39.536440+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.5206","created_at":"2026-05-18T03:00:39.536440+00:00"},{"alias_kind":"pith_short_12","alias_value":"7CWHD76RZMQ6","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"7CWHD76RZMQ6B2A2","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"7CWHD76R","created_at":"2026-05-18T12:27:36.564083+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/7CWHD76RZMQ6B2A23H4VRDBB4I","json":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I.json","graph_json":"https://pith.science/api/pith-number/7CWHD76RZMQ6B2A23H4VRDBB4I/graph.json","events_json":"https://pith.science/api/pith-number/7CWHD76RZMQ6B2A23H4VRDBB4I/events.json","paper":"https://pith.science/paper/7CWHD76R"},"agent_actions":{"view_html":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I","download_json":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I.json","view_paper":"https://pith.science/paper/7CWHD76R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.5206&json=true","fetch_graph":"https://pith.science/api/pith-number/7CWHD76RZMQ6B2A23H4VRDBB4I/graph.json","fetch_events":"https://pith.science/api/pith-number/7CWHD76RZMQ6B2A23H4VRDBB4I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I/action/storage_attestation","attest_author":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I/action/author_attestation","sign_citation":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I/action/citation_signature","submit_replication":"https://pith.science/pith/7CWHD76RZMQ6B2A23H4VRDBB4I/action/replication_record"}},"created_at":"2026-05-18T03:00:39.536440+00:00","updated_at":"2026-05-18T03:00:39.536440+00:00"}