{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:M5QL4QKJVMXMNOTVTTUIQE23PH","short_pith_number":"pith:M5QL4QKJ","schema_version":"1.0","canonical_sha256":"6760be4149ab2ec6ba759ce888135b79ffebaf7e9eb9fe314a8d41d3ef7313c0","source":{"kind":"arxiv","id":"2111.14124","version":2},"attestation_state":"computed","paper":{"title":"Dyon Production from Near-Extremal Kerr-Newman-(Anti-)de Sitter Black Holes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Chiang-Mei Chen, Sang Pyo Kim","submitted_at":"2021-11-28T11:59:50Z","abstract_excerpt":"Using the enhanced symmetry in the near-horizon region of the near-extremal dyonic Kerr-Newman (KN) black hole in the (A)dS space, we find the exact solutions for dyonic charged scalar field in terms of the hypergeometric function and explicitly compute the Schwinger effect for the emission of electric and/or magnetic charges. The emission formula confirms a universal factorization of the Schwinger formula in the AdS$_2$ and another Schwinger formula in the two-dimensional Rindler space determined by the effective temperature and the Hawking temperature with the chemical potentials of electric"},"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":"2111.14124","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-11-28T11:59:50Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d0549e479ec531bdd8d4899907fcb51318edb3750eba64b3c77146544d9dd63e","abstract_canon_sha256":"a356d8dd55cceea1484a7db33f6cd90c03cce3f024c5ec531c023403931ec18f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:51:24.773325Z","signature_b64":"8YGXVEvziyhghZRkr8wzPJ/hK88mvLcqb912wTdEerJzvIpXVqS/+cJYa8zkEv+GUzmlj8Bvpah7ks7BbzooDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6760be4149ab2ec6ba759ce888135b79ffebaf7e9eb9fe314a8d41d3ef7313c0","last_reissued_at":"2026-07-05T05:51:24.772966Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:51:24.772966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dyon Production from Near-Extremal Kerr-Newman-(Anti-)de Sitter Black Holes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Chiang-Mei Chen, Sang Pyo Kim","submitted_at":"2021-11-28T11:59:50Z","abstract_excerpt":"Using the enhanced symmetry in the near-horizon region of the near-extremal dyonic Kerr-Newman (KN) black hole in the (A)dS space, we find the exact solutions for dyonic charged scalar field in terms of the hypergeometric function and explicitly compute the Schwinger effect for the emission of electric and/or magnetic charges. The emission formula confirms a universal factorization of the Schwinger formula in the AdS$_2$ and another Schwinger formula in the two-dimensional Rindler space determined by the effective temperature and the Hawking temperature with the chemical potentials of electric"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.14124","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2111.14124/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2111.14124","created_at":"2026-07-05T05:51:24.773022+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.14124v2","created_at":"2026-07-05T05:51:24.773022+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.14124","created_at":"2026-07-05T05:51:24.773022+00:00"},{"alias_kind":"pith_short_12","alias_value":"M5QL4QKJVMXM","created_at":"2026-07-05T05:51:24.773022+00:00"},{"alias_kind":"pith_short_16","alias_value":"M5QL4QKJVMXMNOTV","created_at":"2026-07-05T05:51:24.773022+00:00"},{"alias_kind":"pith_short_8","alias_value":"M5QL4QKJ","created_at":"2026-07-05T05:51:24.773022+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/M5QL4QKJVMXMNOTVTTUIQE23PH","json":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH.json","graph_json":"https://pith.science/api/pith-number/M5QL4QKJVMXMNOTVTTUIQE23PH/graph.json","events_json":"https://pith.science/api/pith-number/M5QL4QKJVMXMNOTVTTUIQE23PH/events.json","paper":"https://pith.science/paper/M5QL4QKJ"},"agent_actions":{"view_html":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH","download_json":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH.json","view_paper":"https://pith.science/paper/M5QL4QKJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.14124&json=true","fetch_graph":"https://pith.science/api/pith-number/M5QL4QKJVMXMNOTVTTUIQE23PH/graph.json","fetch_events":"https://pith.science/api/pith-number/M5QL4QKJVMXMNOTVTTUIQE23PH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH/action/storage_attestation","attest_author":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH/action/author_attestation","sign_citation":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH/action/citation_signature","submit_replication":"https://pith.science/pith/M5QL4QKJVMXMNOTVTTUIQE23PH/action/replication_record"}},"created_at":"2026-07-05T05:51:24.773022+00:00","updated_at":"2026-07-05T05:51:24.773022+00:00"}