{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:TOSVDUMPZWHVLJFWZNZTWL6EAZ","short_pith_number":"pith:TOSVDUMP","schema_version":"1.0","canonical_sha256":"9ba551d18fcd8f55a4b6cb733b2fc406435ecbaf420e223887cf25eb3c774649","source":{"kind":"arxiv","id":"2401.13749","version":2},"attestation_state":"computed","paper":{"title":"Superconformal Two-Point Functions of the Nahm Pole Defect in $\\mathcal{N}=4$ Super-Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Adam Chalabi, Charlotte Kristjansen, Jonah Baerman","submitted_at":"2024-01-24T19:08:55Z","abstract_excerpt":"We derive a manifestly superconformal expression for the leading-order two-point functions of all single trace chiral primary operators in 4d $\\mathcal{N}=4$ super-Yang-Mills theory with a co-dimension one Nahm pole defect. Notably, our result involves only a finite number of superblocks that correspond to 1/2-BPS representations in the defect channel. The derivation builds on a non-trivial exact result for traces of fuzzy spherical harmonics in combination with powers of $\\mathfrak{su}(2)$ generators, which leads to a remarkably compact expression for the bulk-to-defect couplings. Apart from "},"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":"2401.13749","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-01-24T19:08:55Z","cross_cats_sorted":[],"title_canon_sha256":"02fd5c16715d6cb438d9e4e0388c5dfb9b0839a44925f957859786b488168962","abstract_canon_sha256":"b2d8b68b561ef8541125946e46595e6cf0784a2b48ee39045616149c9077e16c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:41:47.232126Z","signature_b64":"Tj1Po1qR8O5cWdG3atOAa1v+WCw9gIpkzNXg74ZaSYsp8NZ+sCvvV0ncDaj4fVbwqhHZ77EmC44wZvmCAjY6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ba551d18fcd8f55a4b6cb733b2fc406435ecbaf420e223887cf25eb3c774649","last_reissued_at":"2026-07-05T07:41:47.231624Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:41:47.231624Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superconformal Two-Point Functions of the Nahm Pole Defect in $\\mathcal{N}=4$ Super-Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Adam Chalabi, Charlotte Kristjansen, Jonah Baerman","submitted_at":"2024-01-24T19:08:55Z","abstract_excerpt":"We derive a manifestly superconformal expression for the leading-order two-point functions of all single trace chiral primary operators in 4d $\\mathcal{N}=4$ super-Yang-Mills theory with a co-dimension one Nahm pole defect. Notably, our result involves only a finite number of superblocks that correspond to 1/2-BPS representations in the defect channel. The derivation builds on a non-trivial exact result for traces of fuzzy spherical harmonics in combination with powers of $\\mathfrak{su}(2)$ generators, which leads to a remarkably compact expression for the bulk-to-defect couplings. Apart from "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.13749","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/2401.13749/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":"2401.13749","created_at":"2026-07-05T07:41:47.231685+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.13749v2","created_at":"2026-07-05T07:41:47.231685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.13749","created_at":"2026-07-05T07:41:47.231685+00:00"},{"alias_kind":"pith_short_12","alias_value":"TOSVDUMPZWHV","created_at":"2026-07-05T07:41:47.231685+00:00"},{"alias_kind":"pith_short_16","alias_value":"TOSVDUMPZWHVLJFW","created_at":"2026-07-05T07:41:47.231685+00:00"},{"alias_kind":"pith_short_8","alias_value":"TOSVDUMP","created_at":"2026-07-05T07:41:47.231685+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.09132","citing_title":"Chiral algebra correlators of the $6$d, $\\mathcal{N}=(2,0)$ theory with a defect","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ","json":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ.json","graph_json":"https://pith.science/api/pith-number/TOSVDUMPZWHVLJFWZNZTWL6EAZ/graph.json","events_json":"https://pith.science/api/pith-number/TOSVDUMPZWHVLJFWZNZTWL6EAZ/events.json","paper":"https://pith.science/paper/TOSVDUMP"},"agent_actions":{"view_html":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ","download_json":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ.json","view_paper":"https://pith.science/paper/TOSVDUMP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.13749&json=true","fetch_graph":"https://pith.science/api/pith-number/TOSVDUMPZWHVLJFWZNZTWL6EAZ/graph.json","fetch_events":"https://pith.science/api/pith-number/TOSVDUMPZWHVLJFWZNZTWL6EAZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ/action/storage_attestation","attest_author":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ/action/author_attestation","sign_citation":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ/action/citation_signature","submit_replication":"https://pith.science/pith/TOSVDUMPZWHVLJFWZNZTWL6EAZ/action/replication_record"}},"created_at":"2026-07-05T07:41:47.231685+00:00","updated_at":"2026-07-05T07:41:47.231685+00:00"}