{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:QKRDCNQHRZRYVFQUAL272T2HB2","short_pith_number":"pith:QKRDCNQH","schema_version":"1.0","canonical_sha256":"82a23136078e638a961402f5fd4f470eac08fcd8e6758834929d9f836fe5c5c9","source":{"kind":"arxiv","id":"hep-th/9403192","version":2},"attestation_state":"computed","paper":{"title":"Exact Models of Extremal Dyonic 4D Black Hole Solutions of Heterotic String Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clifford V Johnson","submitted_at":"1994-03-31T15:53:16Z","abstract_excerpt":"Families of exact $(0,2)$ supersymmetric conformal field theories of magnetically and electrically charged extremal 4D black hole solutions of heterotic string theory are presented. They are constructed using a $(0,1)$ supersymmetric $SL(2,R)\\times SU(2)$ WZW model where anomalously embedded $U(1)\\times U(1)$ subgroups are gauged. Crucial cancelations of the $U(1)$ anomalies coming from the supersymmetric fermions, the current algebra fermions and the gauging ensure that there is a consistency of these models at the quantum level. Various 2D models, which may be considered as building blocks f"},"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":"hep-th/9403192","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-03-31T15:53:16Z","cross_cats_sorted":[],"title_canon_sha256":"a4ac4fb6b3b0bfea29730b2724ff0547e49072cf98df37c72a609a1236222146","abstract_canon_sha256":"509467ce1f66bd950a704510a29561ad26709736e91816b8039d4a743a7bcb25"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:21.265472Z","signature_b64":"z2tiQsamkcTuVQNRG9jN4GP3kUobo22e9/QVMfu25igNRx4PetdLEttnIlSaweCokaMxtMUEmg1MaFXV3FAKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"82a23136078e638a961402f5fd4f470eac08fcd8e6758834929d9f836fe5c5c9","last_reissued_at":"2026-05-18T03:07:21.264948Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:21.264948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact Models of Extremal Dyonic 4D Black Hole Solutions of Heterotic String Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clifford V Johnson","submitted_at":"1994-03-31T15:53:16Z","abstract_excerpt":"Families of exact $(0,2)$ supersymmetric conformal field theories of magnetically and electrically charged extremal 4D black hole solutions of heterotic string theory are presented. They are constructed using a $(0,1)$ supersymmetric $SL(2,R)\\times SU(2)$ WZW model where anomalously embedded $U(1)\\times U(1)$ subgroups are gauged. Crucial cancelations of the $U(1)$ anomalies coming from the supersymmetric fermions, the current algebra fermions and the gauging ensure that there is a consistency of these models at the quantum level. Various 2D models, which may be considered as building blocks f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9403192","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":"hep-th/9403192","created_at":"2026-05-18T03:07:21.265041+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9403192v2","created_at":"2026-05-18T03:07:21.265041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9403192","created_at":"2026-05-18T03:07:21.265041+00:00"},{"alias_kind":"pith_short_12","alias_value":"QKRDCNQHRZRY","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"QKRDCNQHRZRYVFQU","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"QKRDCNQH","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.15566","citing_title":"One-loop effect in the charged 2D black hole near extremality","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2","json":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2.json","graph_json":"https://pith.science/api/pith-number/QKRDCNQHRZRYVFQUAL272T2HB2/graph.json","events_json":"https://pith.science/api/pith-number/QKRDCNQHRZRYVFQUAL272T2HB2/events.json","paper":"https://pith.science/paper/QKRDCNQH"},"agent_actions":{"view_html":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2","download_json":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2.json","view_paper":"https://pith.science/paper/QKRDCNQH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9403192&json=true","fetch_graph":"https://pith.science/api/pith-number/QKRDCNQHRZRYVFQUAL272T2HB2/graph.json","fetch_events":"https://pith.science/api/pith-number/QKRDCNQHRZRYVFQUAL272T2HB2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2/action/storage_attestation","attest_author":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2/action/author_attestation","sign_citation":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2/action/citation_signature","submit_replication":"https://pith.science/pith/QKRDCNQHRZRYVFQUAL272T2HB2/action/replication_record"}},"created_at":"2026-05-18T03:07:21.265041+00:00","updated_at":"2026-05-18T03:07:21.265041+00:00"}