{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XUTDNNLM5E53U2ZPVOTJQYXXXK","short_pith_number":"pith:XUTDNNLM","schema_version":"1.0","canonical_sha256":"bd2636b56ce93bba6b2faba69862f7ba851a3df4d6508af5f3e1676dcf6a5074","source":{"kind":"arxiv","id":"1710.07336","version":3},"attestation_state":"computed","paper":{"title":"On the Large $R$-charge Expansion in ${\\mathcal N} = 2$ Superconformal Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shunsuke Maeda, Simeon Hellerman","submitted_at":"2017-10-19T19:56:26Z","abstract_excerpt":"In this note we study two point functions of Coulomb branch chiral ring elements with large $R$-charge, in quantum field theories with ${\\mathcal N} = 2$ superconformal symmetry in four spacetime dimensions. Focusing on the case of one-dimensional Coulomb branch, we use the effective-field-theoretic methods of arXiv:1706.05743, to estimate the two-point function $${\\mathcal Y}_n \\equiv |x-y|^{2n\\Delta_{\\mathcal O}}\\left<({\\mathcal O}(x))^n(\\bar{\\mathcal O}(y))^n\\right>$$ in the limit where the operator insertion On has large total $R$-charge ${\\mathcal J} = n\\Delta_{\\mathcal O}$. We show that "},"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":"1710.07336","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-19T19:56:26Z","cross_cats_sorted":[],"title_canon_sha256":"8d4e0d932878179153fe83b0843db028afd1648fdcec992f9b7a7ee109a68794","abstract_canon_sha256":"bf2818dce4f3db79bb41a386c9376aef906c60e7b88caac8b453fca9dac6b695"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:00.097601Z","signature_b64":"shpSSzBtHOx6mZVOj9EWqatLvZiAAkYR+Ge7ic3/jecT4rk7yFORCyrcbyHYvAmWRfsRwuwamaKIL9gT6satCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd2636b56ce93bba6b2faba69862f7ba851a3df4d6508af5f3e1676dcf6a5074","last_reissued_at":"2026-05-18T00:27:00.096940Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:00.096940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the Large $R$-charge Expansion in ${\\mathcal N} = 2$ Superconformal Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shunsuke Maeda, Simeon Hellerman","submitted_at":"2017-10-19T19:56:26Z","abstract_excerpt":"In this note we study two point functions of Coulomb branch chiral ring elements with large $R$-charge, in quantum field theories with ${\\mathcal N} = 2$ superconformal symmetry in four spacetime dimensions. Focusing on the case of one-dimensional Coulomb branch, we use the effective-field-theoretic methods of arXiv:1706.05743, to estimate the two-point function $${\\mathcal Y}_n \\equiv |x-y|^{2n\\Delta_{\\mathcal O}}\\left<({\\mathcal O}(x))^n(\\bar{\\mathcal O}(y))^n\\right>$$ in the limit where the operator insertion On has large total $R$-charge ${\\mathcal J} = n\\Delta_{\\mathcal O}$. We show that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07336","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":""},"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":"1710.07336","created_at":"2026-05-18T00:27:00.097030+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.07336v3","created_at":"2026-05-18T00:27:00.097030+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07336","created_at":"2026-05-18T00:27:00.097030+00:00"},{"alias_kind":"pith_short_12","alias_value":"XUTDNNLM5E53","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"XUTDNNLM5E53U2ZP","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"XUTDNNLM","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2406.19441","citing_title":"Moduli Spaces in CFT: Large Charge Operators","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK","json":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK.json","graph_json":"https://pith.science/api/pith-number/XUTDNNLM5E53U2ZPVOTJQYXXXK/graph.json","events_json":"https://pith.science/api/pith-number/XUTDNNLM5E53U2ZPVOTJQYXXXK/events.json","paper":"https://pith.science/paper/XUTDNNLM"},"agent_actions":{"view_html":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK","download_json":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK.json","view_paper":"https://pith.science/paper/XUTDNNLM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.07336&json=true","fetch_graph":"https://pith.science/api/pith-number/XUTDNNLM5E53U2ZPVOTJQYXXXK/graph.json","fetch_events":"https://pith.science/api/pith-number/XUTDNNLM5E53U2ZPVOTJQYXXXK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK/action/storage_attestation","attest_author":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK/action/author_attestation","sign_citation":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK/action/citation_signature","submit_replication":"https://pith.science/pith/XUTDNNLM5E53U2ZPVOTJQYXXXK/action/replication_record"}},"created_at":"2026-05-18T00:27:00.097030+00:00","updated_at":"2026-05-18T00:27:00.097030+00:00"}