{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:LYCR7ZJEUANTKWNTHSEQLSUXDF","short_pith_number":"pith:LYCR7ZJE","schema_version":"1.0","canonical_sha256":"5e051fe524a01b3559b33c8905ca97194becde3c7b9bc6c3538b6544bd874071","source":{"kind":"arxiv","id":"hep-th/9801066","version":2},"attestation_state":"computed","paper":{"title":"N=4 Supersymmetric Yang-Mills Theory on a Kaehler Surface","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bernd Schroers, Jae-Suk Park, Robbert Dijkgraaf","submitted_at":"1998-01-12T14:32:50Z","abstract_excerpt":"We study N=4 supersymmetric Yang-Mills theory on a Kaehler manifold with $b_2^+ \\geq 3$. Adding suitable perturbations we show that the partition function of the N=4 theory is the sum of contributions from two branches: (i) instantons, (ii) a special class of Seiberg-Witten monopoles. We determine the partition function for the theories with gauge group SU(2) and SO(3), using S-duality. This leads us to a formula for the Euler characteristic of the moduli space of instantons."},"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/9801066","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-01-12T14:32:50Z","cross_cats_sorted":[],"title_canon_sha256":"ba17d9d48642b8f2711a082ce52c6b05594792ff123978f46dba289c68cf52e9","abstract_canon_sha256":"acee36e1003450aac5dbb5b2871b17da23a97dab45bbca656f0ba8459a78fd9f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:33:10.063742Z","signature_b64":"h9+ot9qQXLuO79DdtE4j2uJovaEtNyvTPh5R52/Zl6T0JVyBhSHZHUd2RfgViCN/DFcbfiOVDxhmdyvR/CdlDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e051fe524a01b3559b33c8905ca97194becde3c7b9bc6c3538b6544bd874071","last_reissued_at":"2026-07-04T14:33:10.063412Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:33:10.063412Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N=4 Supersymmetric Yang-Mills Theory on a Kaehler Surface","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bernd Schroers, Jae-Suk Park, Robbert Dijkgraaf","submitted_at":"1998-01-12T14:32:50Z","abstract_excerpt":"We study N=4 supersymmetric Yang-Mills theory on a Kaehler manifold with $b_2^+ \\geq 3$. Adding suitable perturbations we show that the partition function of the N=4 theory is the sum of contributions from two branches: (i) instantons, (ii) a special class of Seiberg-Witten monopoles. We determine the partition function for the theories with gauge group SU(2) and SO(3), using S-duality. This leads us to a formula for the Euler characteristic of the moduli space of instantons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9801066","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/hep-th/9801066/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/9801066","created_at":"2026-07-04T14:33:10.063462+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9801066v2","created_at":"2026-07-04T14:33:10.063462+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9801066","created_at":"2026-07-04T14:33:10.063462+00:00"},{"alias_kind":"pith_short_12","alias_value":"LYCR7ZJEUANT","created_at":"2026-07-04T14:33:10.063462+00:00"},{"alias_kind":"pith_short_16","alias_value":"LYCR7ZJEUANTKWNT","created_at":"2026-07-04T14:33:10.063462+00:00"},{"alias_kind":"pith_short_8","alias_value":"LYCR7ZJE","created_at":"2026-07-04T14:33:10.063462+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.23481","citing_title":"Central Charges and Vacuum Moduli of 2d $\\mathcal{N}=(0,4)$ Theories from Class $\\mathcal{S}$","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF","json":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF.json","graph_json":"https://pith.science/api/pith-number/LYCR7ZJEUANTKWNTHSEQLSUXDF/graph.json","events_json":"https://pith.science/api/pith-number/LYCR7ZJEUANTKWNTHSEQLSUXDF/events.json","paper":"https://pith.science/paper/LYCR7ZJE"},"agent_actions":{"view_html":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF","download_json":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF.json","view_paper":"https://pith.science/paper/LYCR7ZJE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9801066&json=true","fetch_graph":"https://pith.science/api/pith-number/LYCR7ZJEUANTKWNTHSEQLSUXDF/graph.json","fetch_events":"https://pith.science/api/pith-number/LYCR7ZJEUANTKWNTHSEQLSUXDF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF/action/storage_attestation","attest_author":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF/action/author_attestation","sign_citation":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF/action/citation_signature","submit_replication":"https://pith.science/pith/LYCR7ZJEUANTKWNTHSEQLSUXDF/action/replication_record"}},"created_at":"2026-07-04T14:33:10.063462+00:00","updated_at":"2026-07-04T14:33:10.063462+00:00"}