{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:VUAY4W7VEXSUIZMWMCEAYGL6ZJ","short_pith_number":"pith:VUAY4W7V","schema_version":"1.0","canonical_sha256":"ad018e5bf525e544659660880c197eca4a455e579f6fa75b5d0244ac1fd38a18","source":{"kind":"arxiv","id":"2211.11795","version":2},"attestation_state":"computed","paper":{"title":"Strong coupling expansions in $\\mathcal{N}=2$ quiver gauge theories","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":"2022-11-21T19:01:02Z","abstract_excerpt":"We study the 3-point functions of gauge-invariant scalar operators in four dimensional $\\mathcal{N}=2$ superconformal quiver theories using supersymmetric localization in the planar limit of a large number of colors. By exploiting a web of nontrivial relations, we show that the 3-point functions can be expressed in terms of the 2-point functions through exact Ward-like identities that are valid for all values of the coupling constant. In this way, using recent results about the 2-point functions, we are able to obtain the asymptotic strong-coupling expansion of the 3-point functions and of 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":"2211.11795","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-11-21T19:01:02Z","cross_cats_sorted":[],"title_canon_sha256":"3aa2163b4f8677ba945e43e78154da348ef08bf6fead3de2a76fa15439c9a2f6","abstract_canon_sha256":"fc47eeff48e22af42c8aecbca56df4501cb68c5217e1b47e462c776f16eac5e3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:39:25.767375Z","signature_b64":"waciPaFJri8zJXn1MWJ/cAUIJMDCZUHd/Q1qfs/FTejwuh9iFwug6d7w848FCVQGTV6kMpueKvn3FJMEJ3oXAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad018e5bf525e544659660880c197eca4a455e579f6fa75b5d0244ac1fd38a18","last_reissued_at":"2026-07-05T05:39:25.766911Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:39:25.766911Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong coupling expansions in $\\mathcal{N}=2$ quiver gauge theories","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":"2022-11-21T19:01:02Z","abstract_excerpt":"We study the 3-point functions of gauge-invariant scalar operators in four dimensional $\\mathcal{N}=2$ superconformal quiver theories using supersymmetric localization in the planar limit of a large number of colors. By exploiting a web of nontrivial relations, we show that the 3-point functions can be expressed in terms of the 2-point functions through exact Ward-like identities that are valid for all values of the coupling constant. In this way, using recent results about the 2-point functions, we are able to obtain the asymptotic strong-coupling expansion of the 3-point functions and of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.11795","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/2211.11795/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":"2211.11795","created_at":"2026-07-05T05:39:25.766970+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.11795v2","created_at":"2026-07-05T05:39:25.766970+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.11795","created_at":"2026-07-05T05:39:25.766970+00:00"},{"alias_kind":"pith_short_12","alias_value":"VUAY4W7VEXSU","created_at":"2026-07-05T05:39:25.766970+00:00"},{"alias_kind":"pith_short_16","alias_value":"VUAY4W7VEXSUIZMW","created_at":"2026-07-05T05:39:25.766970+00:00"},{"alias_kind":"pith_short_8","alias_value":"VUAY4W7V","created_at":"2026-07-05T05:39:25.766970+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":40,"is_internal_anchor":false},{"citing_arxiv_id":"2512.16984","citing_title":"Exploring the twisted sector of $\\mathbb{Z}_{L}$ orbifolds: Matching $\\alpha'$-corrections to localisation","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ","json":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ.json","graph_json":"https://pith.science/api/pith-number/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/graph.json","events_json":"https://pith.science/api/pith-number/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/events.json","paper":"https://pith.science/paper/VUAY4W7V"},"agent_actions":{"view_html":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ","download_json":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ.json","view_paper":"https://pith.science/paper/VUAY4W7V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.11795&json=true","fetch_graph":"https://pith.science/api/pith-number/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/graph.json","fetch_events":"https://pith.science/api/pith-number/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/action/storage_attestation","attest_author":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/action/author_attestation","sign_citation":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/action/citation_signature","submit_replication":"https://pith.science/pith/VUAY4W7VEXSUIZMWMCEAYGL6ZJ/action/replication_record"}},"created_at":"2026-07-05T05:39:25.766970+00:00","updated_at":"2026-07-05T05:39:25.766970+00:00"}