{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:Y7GRZLO3IE6WZI33TEFUYQWHKA","short_pith_number":"pith:Y7GRZLO3","schema_version":"1.0","canonical_sha256":"c7cd1caddb413d6ca37b990b4c42c750152627a2cccf84e4f36c68746c404c24","source":{"kind":"arxiv","id":"2202.06990","version":3},"attestation_state":"computed","paper":{"title":"Three-point functions in a $\\mathcal{N}=2$ superconformal gauge theory and their strong-coupling limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Lerda, A. Pini, M. Billo, M. Frau, P. Vallarino","submitted_at":"2022-02-14T19:05:56Z","abstract_excerpt":"We study the 3-point functions of single-trace scalar operators in a four-dimensional $\\mathcal{N}=2$ SYM theory with gauge group $\\mathrm{SU}(N)$ and matter in the symmetric plus anti-symmetric representation, which has a vanishing $\\beta$-function. By mapping this computation to the matrix model arising from localization on a 4-sphere we are able to resum the perturbative expansion in the large-$N$ 't Hooft limit and derive the behavior of the correlators at strong coupling. Finally, by combining our results on the 3-point functions with those on the 2-point functions that have been recently"},"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":"2202.06990","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-02-14T19:05:56Z","cross_cats_sorted":[],"title_canon_sha256":"4ea377165c6deb9143e8bd83d4bf8cc46e82d10610dabb9af33cfefed5ed98e5","abstract_canon_sha256":"dfe34a98eed1e4e864fa5c3ff281695adfb1a7522d2448e1abd7773e9e295dd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:54:52.425228Z","signature_b64":"BXNy2WmzvH1S3fueWa7V/4vrW38lK1627e93PF87tGwd/OifyyGJhArqzgABEqTkIxD+/Pv1LTqQtk3O7cLlCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7cd1caddb413d6ca37b990b4c42c750152627a2cccf84e4f36c68746c404c24","last_reissued_at":"2026-07-05T04:54:52.424763Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:54:52.424763Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-point functions in a $\\mathcal{N}=2$ superconformal gauge theory and their strong-coupling limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Lerda, A. Pini, M. Billo, M. Frau, P. Vallarino","submitted_at":"2022-02-14T19:05:56Z","abstract_excerpt":"We study the 3-point functions of single-trace scalar operators in a four-dimensional $\\mathcal{N}=2$ SYM theory with gauge group $\\mathrm{SU}(N)$ and matter in the symmetric plus anti-symmetric representation, which has a vanishing $\\beta$-function. By mapping this computation to the matrix model arising from localization on a 4-sphere we are able to resum the perturbative expansion in the large-$N$ 't Hooft limit and derive the behavior of the correlators at strong coupling. Finally, by combining our results on the 3-point functions with those on the 2-point functions that have been recently"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.06990","kind":"arxiv","version":3},"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/2202.06990/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":"2202.06990","created_at":"2026-07-05T04:54:52.424820+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.06990v3","created_at":"2026-07-05T04:54:52.424820+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.06990","created_at":"2026-07-05T04:54:52.424820+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y7GRZLO3IE6W","created_at":"2026-07-05T04:54:52.424820+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y7GRZLO3IE6WZI33","created_at":"2026-07-05T04:54:52.424820+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y7GRZLO3","created_at":"2026-07-05T04:54:52.424820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.24101","citing_title":"Bremsstrahlung function in $\\mathcal{N}=2$ SCFTs far beyond the supergravity limit","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16521","citing_title":"Strong-coupling results in (non-)conformal $\\mathcal{N}=2$ theories with fundamental flavors","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA","json":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA.json","graph_json":"https://pith.science/api/pith-number/Y7GRZLO3IE6WZI33TEFUYQWHKA/graph.json","events_json":"https://pith.science/api/pith-number/Y7GRZLO3IE6WZI33TEFUYQWHKA/events.json","paper":"https://pith.science/paper/Y7GRZLO3"},"agent_actions":{"view_html":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA","download_json":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA.json","view_paper":"https://pith.science/paper/Y7GRZLO3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.06990&json=true","fetch_graph":"https://pith.science/api/pith-number/Y7GRZLO3IE6WZI33TEFUYQWHKA/graph.json","fetch_events":"https://pith.science/api/pith-number/Y7GRZLO3IE6WZI33TEFUYQWHKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA/action/storage_attestation","attest_author":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA/action/author_attestation","sign_citation":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA/action/citation_signature","submit_replication":"https://pith.science/pith/Y7GRZLO3IE6WZI33TEFUYQWHKA/action/replication_record"}},"created_at":"2026-07-05T04:54:52.424820+00:00","updated_at":"2026-07-05T04:54:52.424820+00:00"}