{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:24SGQIL7ATFR746VSSYUVUHE7T","short_pith_number":"pith:24SGQIL7","schema_version":"1.0","canonical_sha256":"d72468217f04cb1ff3d594b14ad0e4fcd9b6f563ff6cbd1442630132c1f4a51a","source":{"kind":"arxiv","id":"1702.04998","version":2},"attestation_state":"computed","paper":{"title":"A string realisation of $\\varOmega$-deformed Abelian $\\mathcal{N}=2^*$ theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Carlo Angelantonj, Ignatios Antoniadis, Marine Samsonyan","submitted_at":"2017-02-16T14:55:35Z","abstract_excerpt":"The $\\mathscr{N}=2^*$ supersymmetric gauge theory is a massive deformation of $\\mathscr{N}=4$, in which the adjoint hypermultiplet gets a mass. We present a D-brane realisation of the (non-)Abelian $\\mathscr{N}=2^*$ theory, and compute suitable topological amplitudes, which are expressed as a double series expansion. The coefficients determine couplings of higher-dimensional operators in the effective supergravity action that involve powers of the anti-self-dual $\\mathscr{N}=2$ chiral Weyl superfield and of self-dual gauge field strengths superpartners of the D5-brane coupling modulus. In the "},"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":"1702.04998","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-16T14:55:35Z","cross_cats_sorted":[],"title_canon_sha256":"5767561bbb8b745dc7618e0ef266753fa8b163d4c478a059ebeee34da83d6589","abstract_canon_sha256":"7f34dec51cceed09d66b015585e220ec83a34be1d916654292110e59bff304b0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:28.829476Z","signature_b64":"mseMd3PmDMMIlNDo4E7fhwD/NLL2oDNLSir8Tv1joe0CNuX6Zty0/+MllDWfR59R9gJK9E9Px8eeujFw5p7pCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d72468217f04cb1ff3d594b14ad0e4fcd9b6f563ff6cbd1442630132c1f4a51a","last_reissued_at":"2026-05-18T00:21:28.828720Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:28.828720Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A string realisation of $\\varOmega$-deformed Abelian $\\mathcal{N}=2^*$ theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Carlo Angelantonj, Ignatios Antoniadis, Marine Samsonyan","submitted_at":"2017-02-16T14:55:35Z","abstract_excerpt":"The $\\mathscr{N}=2^*$ supersymmetric gauge theory is a massive deformation of $\\mathscr{N}=4$, in which the adjoint hypermultiplet gets a mass. We present a D-brane realisation of the (non-)Abelian $\\mathscr{N}=2^*$ theory, and compute suitable topological amplitudes, which are expressed as a double series expansion. The coefficients determine couplings of higher-dimensional operators in the effective supergravity action that involve powers of the anti-self-dual $\\mathscr{N}=2$ chiral Weyl superfield and of self-dual gauge field strengths superpartners of the D5-brane coupling modulus. In the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.04998","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":"1702.04998","created_at":"2026-05-18T00:21:28.828841+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.04998v2","created_at":"2026-05-18T00:21:28.828841+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.04998","created_at":"2026-05-18T00:21:28.828841+00:00"},{"alias_kind":"pith_short_12","alias_value":"24SGQIL7ATFR","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"24SGQIL7ATFR746V","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"24SGQIL7","created_at":"2026-05-18T12:30:55.937587+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/24SGQIL7ATFR746VSSYUVUHE7T","json":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T.json","graph_json":"https://pith.science/api/pith-number/24SGQIL7ATFR746VSSYUVUHE7T/graph.json","events_json":"https://pith.science/api/pith-number/24SGQIL7ATFR746VSSYUVUHE7T/events.json","paper":"https://pith.science/paper/24SGQIL7"},"agent_actions":{"view_html":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T","download_json":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T.json","view_paper":"https://pith.science/paper/24SGQIL7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.04998&json=true","fetch_graph":"https://pith.science/api/pith-number/24SGQIL7ATFR746VSSYUVUHE7T/graph.json","fetch_events":"https://pith.science/api/pith-number/24SGQIL7ATFR746VSSYUVUHE7T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T/action/storage_attestation","attest_author":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T/action/author_attestation","sign_citation":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T/action/citation_signature","submit_replication":"https://pith.science/pith/24SGQIL7ATFR746VSSYUVUHE7T/action/replication_record"}},"created_at":"2026-05-18T00:21:28.828841+00:00","updated_at":"2026-05-18T00:21:28.828841+00:00"}