{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:NXLKVWF2EAFZWXJD4GGXQPWZOR","short_pith_number":"pith:NXLKVWF2","schema_version":"1.0","canonical_sha256":"6dd6aad8ba200b9b5d23e18d783ed974649cdf03e776457f3a7d905583c54493","source":{"kind":"arxiv","id":"hep-th/9608047","version":1},"attestation_state":"computed","paper":{"title":"An N=2 Superconformal Fixed Point with E_6 Global Symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dennis Nemeschansky, Joseph A. Minahan","submitted_at":"1996-08-08T18:05:36Z","abstract_excerpt":"We obtain the elliptic curve corresponding to an $N=2$ superconformal field theory which has an $E_6$ global symmetry at the strong coupling point $\\tau=e^{\\pi i/3}$. We also find the Seiberg-Witten differential $\\lambda_{SW}$ for this theory. This differential has 27 poles corresponding to the fundamental representation of $E_6$. The complex conjugate representation has its poles on the other sheet. We also show that the $E_6$ curve reduces to the $D_4$ curve of Seiberg and Witten. Finally, we compute the monodromies and use these to compute BPS masses in an $F$-Theory compactification."},"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/9608047","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-08-08T18:05:36Z","cross_cats_sorted":[],"title_canon_sha256":"8717a08abae3c5d6945fe73498564ba0dca9ca972393c0aa284eb09f67b4e495","abstract_canon_sha256":"ae6217544eee237a03e90bbc586e48dafb35111a47f864027ea12e62e75b423f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:20.766729Z","signature_b64":"lbx5AfYSQmM1bLQihQ+hMPYeg0cqsIEA9xsfGhggZtmxO3xgHMt5sVYVbBHhrcn07vWq1yEqjwSv1FUviHCPAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6dd6aad8ba200b9b5d23e18d783ed974649cdf03e776457f3a7d905583c54493","last_reissued_at":"2026-07-04T16:02:20.766398Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:20.766398Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An N=2 Superconformal Fixed Point with E_6 Global Symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dennis Nemeschansky, Joseph A. Minahan","submitted_at":"1996-08-08T18:05:36Z","abstract_excerpt":"We obtain the elliptic curve corresponding to an $N=2$ superconformal field theory which has an $E_6$ global symmetry at the strong coupling point $\\tau=e^{\\pi i/3}$. We also find the Seiberg-Witten differential $\\lambda_{SW}$ for this theory. This differential has 27 poles corresponding to the fundamental representation of $E_6$. The complex conjugate representation has its poles on the other sheet. We also show that the $E_6$ curve reduces to the $D_4$ curve of Seiberg and Witten. Finally, we compute the monodromies and use these to compute BPS masses in an $F$-Theory compactification."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9608047","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/9608047/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/9608047","created_at":"2026-07-04T16:02:20.766454+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9608047v1","created_at":"2026-07-04T16:02:20.766454+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9608047","created_at":"2026-07-04T16:02:20.766454+00:00"},{"alias_kind":"pith_short_12","alias_value":"NXLKVWF2EAFZ","created_at":"2026-07-04T16:02:20.766454+00:00"},{"alias_kind":"pith_short_16","alias_value":"NXLKVWF2EAFZWXJD","created_at":"2026-07-04T16:02:20.766454+00:00"},{"alias_kind":"pith_short_8","alias_value":"NXLKVWF2","created_at":"2026-07-04T16:02:20.766454+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2412.03588","citing_title":"Spectral Networks: Bridging higher-rank Teichm\\\"uller theory and BPS states","ref_index":274,"is_internal_anchor":true},{"citing_arxiv_id":"2603.19168","citing_title":"Quasinormal Modes of Extremal Reissner-Nordstrom Black Holes via Seiberg-Witten Quantization","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR","json":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR.json","graph_json":"https://pith.science/api/pith-number/NXLKVWF2EAFZWXJD4GGXQPWZOR/graph.json","events_json":"https://pith.science/api/pith-number/NXLKVWF2EAFZWXJD4GGXQPWZOR/events.json","paper":"https://pith.science/paper/NXLKVWF2"},"agent_actions":{"view_html":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR","download_json":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR.json","view_paper":"https://pith.science/paper/NXLKVWF2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9608047&json=true","fetch_graph":"https://pith.science/api/pith-number/NXLKVWF2EAFZWXJD4GGXQPWZOR/graph.json","fetch_events":"https://pith.science/api/pith-number/NXLKVWF2EAFZWXJD4GGXQPWZOR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR/action/storage_attestation","attest_author":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR/action/author_attestation","sign_citation":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR/action/citation_signature","submit_replication":"https://pith.science/pith/NXLKVWF2EAFZWXJD4GGXQPWZOR/action/replication_record"}},"created_at":"2026-07-04T16:02:20.766454+00:00","updated_at":"2026-07-04T16:02:20.766454+00:00"}