{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1992:RWEZZFUFJ523II7H5CZHALJI7S","short_pith_number":"pith:RWEZZFUF","schema_version":"1.0","canonical_sha256":"8d899c96854f75b423e7e8b2702d28fcb67405ef4c28947d490b343c41238abf","source":{"kind":"arxiv","id":"hep-th/9212062","version":1},"attestation_state":"computed","paper":{"title":"Notes on N=2 $\\sigma$-models$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. Distler","submitted_at":"1992-12-10T06:22:34Z","abstract_excerpt":"These lectures, given at the 1992 Trieste Spring School, are devoted to some selected topics in N=2 \\sm s on Calabi-Yau manifolds and the associated N=2 superconformal field theories. The first lecture is devoted to the ``special geometry\" of the moduli space of $c=9$ N=2 superconformal field theories. An important role is played by the extended chiral algebra which appears in theories with integer $U(1)$ charges. The second lecture is devoted to the \\sm\\ approach. The main focus is an explication of a calculation of Aspinwall and Morrison."},"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/9212062","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1992-12-10T06:22:34Z","cross_cats_sorted":[],"title_canon_sha256":"df837b3bb0b704e639db1263e055cd78e60ea189f2c0da3c40f9e528af5a4e19","abstract_canon_sha256":"698304c12f209542d409347696ba81b5c51116f716c6407f43ad098778a00c15"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:32:28.529028Z","signature_b64":"kOhw2Wn+0OL4Yay7tRyPiBQJY246L/+mK6/K3pKelV5KIbyYSy21HxGPqewSIQYLxVk0gMRK1HJaWyifhpV4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d899c96854f75b423e7e8b2702d28fcb67405ef4c28947d490b343c41238abf","last_reissued_at":"2026-07-04T14:32:28.528709Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:32:28.528709Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Notes on N=2 $\\sigma$-models$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"J. Distler","submitted_at":"1992-12-10T06:22:34Z","abstract_excerpt":"These lectures, given at the 1992 Trieste Spring School, are devoted to some selected topics in N=2 \\sm s on Calabi-Yau manifolds and the associated N=2 superconformal field theories. The first lecture is devoted to the ``special geometry\" of the moduli space of $c=9$ N=2 superconformal field theories. An important role is played by the extended chiral algebra which appears in theories with integer $U(1)$ charges. The second lecture is devoted to the \\sm\\ approach. The main focus is an explication of a calculation of Aspinwall and Morrison."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9212062","kind":"arxiv","version":1},"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/hep-th/9212062/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":"hep-th/9212062","created_at":"2026-07-04T14:32:28.528761+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9212062v1","created_at":"2026-07-04T14:32:28.528761+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9212062","created_at":"2026-07-04T14:32:28.528761+00:00"},{"alias_kind":"pith_short_12","alias_value":"RWEZZFUFJ523","created_at":"2026-07-04T14:32:28.528761+00:00"},{"alias_kind":"pith_short_16","alias_value":"RWEZZFUFJ523II7H","created_at":"2026-07-04T14:32:28.528761+00:00"},{"alias_kind":"pith_short_8","alias_value":"RWEZZFUF","created_at":"2026-07-04T14:32:28.528761+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.12525","citing_title":"Higher Structures on Boundary Conformal Manifolds: Higher Berry Phase and Boundary Conformal Field Theory","ref_index":144,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S","json":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S.json","graph_json":"https://pith.science/api/pith-number/RWEZZFUFJ523II7H5CZHALJI7S/graph.json","events_json":"https://pith.science/api/pith-number/RWEZZFUFJ523II7H5CZHALJI7S/events.json","paper":"https://pith.science/paper/RWEZZFUF"},"agent_actions":{"view_html":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S","download_json":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S.json","view_paper":"https://pith.science/paper/RWEZZFUF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9212062&json=true","fetch_graph":"https://pith.science/api/pith-number/RWEZZFUFJ523II7H5CZHALJI7S/graph.json","fetch_events":"https://pith.science/api/pith-number/RWEZZFUFJ523II7H5CZHALJI7S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S/action/storage_attestation","attest_author":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S/action/author_attestation","sign_citation":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S/action/citation_signature","submit_replication":"https://pith.science/pith/RWEZZFUFJ523II7H5CZHALJI7S/action/replication_record"}},"created_at":"2026-07-04T14:32:28.528761+00:00","updated_at":"2026-07-04T14:32:28.528761+00:00"}