{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:RODHEPCYDYOL25KUSZZG4HDG3T","short_pith_number":"pith:RODHEPCY","schema_version":"1.0","canonical_sha256":"8b86723c581e1cbd755496726e1c66dce07b8fe510a79c03bdd727a322134087","source":{"kind":"arxiv","id":"1312.4453","version":2},"attestation_state":"computed","paper":{"title":"Quantum probes of timelike naked singularities in the weak field regime of $f(R)$ global monopole spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M. Halilsoy, O. Gurtug, S. Habib Mazharimousavi","submitted_at":"2013-12-16T18:39:04Z","abstract_excerpt":"The formation of a naked singularity in $f(R)$ global monopole spacetime is considered in view of quantum mechanics. Quantum test fields obeying the Klein$-$Gordon, Dirac and Maxwell equations are used to probe the classical timelike naked singularity developed at $r=0$. We prove that the spatial derivative operator of the fields fails to be essentially self-adjoint. As a result, the classical timelike naked singularity formed in $f(R)$ global monopole spacetime remains quantum mechanically singular when it is probed with quantum fields having different spin structures. Pitelli and Letelier (P"},"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":"1312.4453","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-16T18:39:04Z","cross_cats_sorted":[],"title_canon_sha256":"ae8ed95f74671de6161d1b27b0b5f31a820f552ba5e00dbc36d3c8fffd649a0d","abstract_canon_sha256":"83a04c0724ce9cf324741132975d4ddc4efa87d04e3d34c2e0979df3efe3276f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:25.404215Z","signature_b64":"OEriaTltKCvyRisuOxoK4G8wPkKOd/LyH9X4v1qTMUFZQNn9hVuKxH58DH2jCSK32puSOdMnP19shCBOWZfWAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b86723c581e1cbd755496726e1c66dce07b8fe510a79c03bdd727a322134087","last_reissued_at":"2026-05-18T03:00:25.403360Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:25.403360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum probes of timelike naked singularities in the weak field regime of $f(R)$ global monopole spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"M. Halilsoy, O. Gurtug, S. Habib Mazharimousavi","submitted_at":"2013-12-16T18:39:04Z","abstract_excerpt":"The formation of a naked singularity in $f(R)$ global monopole spacetime is considered in view of quantum mechanics. Quantum test fields obeying the Klein$-$Gordon, Dirac and Maxwell equations are used to probe the classical timelike naked singularity developed at $r=0$. We prove that the spatial derivative operator of the fields fails to be essentially self-adjoint. As a result, the classical timelike naked singularity formed in $f(R)$ global monopole spacetime remains quantum mechanically singular when it is probed with quantum fields having different spin structures. Pitelli and Letelier (P"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.4453","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":"1312.4453","created_at":"2026-05-18T03:00:25.403479+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.4453v2","created_at":"2026-05-18T03:00:25.403479+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.4453","created_at":"2026-05-18T03:00:25.403479+00:00"},{"alias_kind":"pith_short_12","alias_value":"RODHEPCYDYOL","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"RODHEPCYDYOL25KU","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"RODHEPCY","created_at":"2026-05-18T12:27:59.945178+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/RODHEPCYDYOL25KUSZZG4HDG3T","json":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T.json","graph_json":"https://pith.science/api/pith-number/RODHEPCYDYOL25KUSZZG4HDG3T/graph.json","events_json":"https://pith.science/api/pith-number/RODHEPCYDYOL25KUSZZG4HDG3T/events.json","paper":"https://pith.science/paper/RODHEPCY"},"agent_actions":{"view_html":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T","download_json":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T.json","view_paper":"https://pith.science/paper/RODHEPCY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.4453&json=true","fetch_graph":"https://pith.science/api/pith-number/RODHEPCYDYOL25KUSZZG4HDG3T/graph.json","fetch_events":"https://pith.science/api/pith-number/RODHEPCYDYOL25KUSZZG4HDG3T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T/action/storage_attestation","attest_author":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T/action/author_attestation","sign_citation":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T/action/citation_signature","submit_replication":"https://pith.science/pith/RODHEPCYDYOL25KUSZZG4HDG3T/action/replication_record"}},"created_at":"2026-05-18T03:00:25.403479+00:00","updated_at":"2026-05-18T03:00:25.403479+00:00"}