{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:VFXXIT7OYQGPQGWMFWTXCL54Z6","short_pith_number":"pith:VFXXIT7O","schema_version":"1.0","canonical_sha256":"a96f744feec40cf81acc2da7712fbccf9bd69382ea5dc2ce6e3c1b2c2086d673","source":{"kind":"arxiv","id":"2103.09312","version":2},"attestation_state":"computed","paper":{"title":"On the exponentially small corrections to ${\\cal N} = 2$ superconformal correlators at large R-charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Simeon Hellerman","submitted_at":"2021-03-16T20:43:55Z","abstract_excerpt":"In this note we consider Coulomb-branch chiral primary correlation functions in ${\\cal N} = 2$ superconformal QCD with gauge group $SU(2)$, in the limit of large R-charge ${\\cal J} = 2n$ for the chiral primary operators $[{\\cal O}(x)]^ n$ with the inverse gauge coupling $\\tau$ held fixed. In previous work, these correlation functions were determined to all orders in $n$, up to unknown exponentially small corrections. In this paper we determine the first several orders of the asymptotic expansion of the exponentially small correction itself. To do this we use: the physical interpretation 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":"2103.09312","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-03-16T20:43:55Z","cross_cats_sorted":[],"title_canon_sha256":"16bd2debb93bfef5f04fbce193c24db40c6e3e22fb57b491c548ab90bdf1bcd8","abstract_canon_sha256":"75ebf2f5c63544116c09b8911ea16ac1e58a90e687035b9afa60f0d21c2a8456"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:24:55.028385Z","signature_b64":"mHadagXXIjJcWG20oCtCkXLgKCOXgt107M/DDjYDJ0mXy9z8ULsb+FIaiBKEwupwo9mTx68QwzXYVDV8cLINDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a96f744feec40cf81acc2da7712fbccf9bd69382ea5dc2ce6e3c1b2c2086d673","last_reissued_at":"2026-07-05T02:24:55.028015Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:24:55.028015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the exponentially small corrections to ${\\cal N} = 2$ superconformal correlators at large R-charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Simeon Hellerman","submitted_at":"2021-03-16T20:43:55Z","abstract_excerpt":"In this note we consider Coulomb-branch chiral primary correlation functions in ${\\cal N} = 2$ superconformal QCD with gauge group $SU(2)$, in the limit of large R-charge ${\\cal J} = 2n$ for the chiral primary operators $[{\\cal O}(x)]^ n$ with the inverse gauge coupling $\\tau$ held fixed. In previous work, these correlation functions were determined to all orders in $n$, up to unknown exponentially small corrections. In this paper we determine the first several orders of the asymptotic expansion of the exponentially small correction itself. To do this we use: the physical interpretation of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.09312","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/2103.09312/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":"2103.09312","created_at":"2026-07-05T02:24:55.028078+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.09312v2","created_at":"2026-07-05T02:24:55.028078+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.09312","created_at":"2026-07-05T02:24:55.028078+00:00"},{"alias_kind":"pith_short_12","alias_value":"VFXXIT7OYQGP","created_at":"2026-07-05T02:24:55.028078+00:00"},{"alias_kind":"pith_short_16","alias_value":"VFXXIT7OYQGPQGWM","created_at":"2026-07-05T02:24:55.028078+00:00"},{"alias_kind":"pith_short_8","alias_value":"VFXXIT7O","created_at":"2026-07-05T02:24:55.028078+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2406.19441","citing_title":"Moduli Spaces in CFT: Large Charge Operators","ref_index":41,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6","json":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6.json","graph_json":"https://pith.science/api/pith-number/VFXXIT7OYQGPQGWMFWTXCL54Z6/graph.json","events_json":"https://pith.science/api/pith-number/VFXXIT7OYQGPQGWMFWTXCL54Z6/events.json","paper":"https://pith.science/paper/VFXXIT7O"},"agent_actions":{"view_html":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6","download_json":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6.json","view_paper":"https://pith.science/paper/VFXXIT7O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.09312&json=true","fetch_graph":"https://pith.science/api/pith-number/VFXXIT7OYQGPQGWMFWTXCL54Z6/graph.json","fetch_events":"https://pith.science/api/pith-number/VFXXIT7OYQGPQGWMFWTXCL54Z6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6/action/storage_attestation","attest_author":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6/action/author_attestation","sign_citation":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6/action/citation_signature","submit_replication":"https://pith.science/pith/VFXXIT7OYQGPQGWMFWTXCL54Z6/action/replication_record"}},"created_at":"2026-07-05T02:24:55.028078+00:00","updated_at":"2026-07-05T02:24:55.028078+00:00"}