{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:VWNQJEHQAWOSHLG76HNL73Z6MS","short_pith_number":"pith:VWNQJEHQ","schema_version":"1.0","canonical_sha256":"ad9b0490f0059d23acdff1dabfef3e64adfdec50d92fbbe6f9a9aebb7244705f","source":{"kind":"arxiv","id":"hep-th/0107084","version":2},"attestation_state":"computed","paper":{"title":"(2,0) Superconformal OPEs in D=6, Selection Rules and Non-renormalization Theorems","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Eden, E. Sokatchev, S. Ferrara","submitted_at":"2001-07-10T19:52:15Z","abstract_excerpt":"We analyse the OPE of any two 1/2 BPS operators of (2,0) SCFT$_6$ by constructing all possible three-point functions that they can form with another, in general long operator. Such three-point functions are uniquely determined by superconformal symmetry. Selection rules are derived, which allow us to infer ``non-renormalization theorems'' for an abstract superconformal field theory. The latter is supposedly related to the strong-coupling dynamics of $N_c$ coincident M5 branes, dual, in the large-$N_c$ limit, to the bulk M-theory compactified on AdS$_7 \\times$S$_4$. An interpretation of extrema"},"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":"hep-th/0107084","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-07-10T19:52:15Z","cross_cats_sorted":[],"title_canon_sha256":"c2e64980c3e73db25b5c18a870436db4512d50f938f123f8dd2fabfcbc684bb0","abstract_canon_sha256":"41d22f7dd790fd9461ff54bc15e47e68b088b882177d5b5475f4835d4de3d287"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:21:05.988483Z","signature_b64":"weGIdP0EYwJes7mVj+JO/i5SF1hwN/K0QnzZemtm9wMYXE2yYmsGuD3bYCqlkXk3nUrH2o37VJRb4jLLLoCQAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad9b0490f0059d23acdff1dabfef3e64adfdec50d92fbbe6f9a9aebb7244705f","last_reissued_at":"2026-07-04T17:21:05.988079Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:21:05.988079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"(2,0) Superconformal OPEs in D=6, Selection Rules and Non-renormalization Theorems","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Eden, E. Sokatchev, S. Ferrara","submitted_at":"2001-07-10T19:52:15Z","abstract_excerpt":"We analyse the OPE of any two 1/2 BPS operators of (2,0) SCFT$_6$ by constructing all possible three-point functions that they can form with another, in general long operator. Such three-point functions are uniquely determined by superconformal symmetry. Selection rules are derived, which allow us to infer ``non-renormalization theorems'' for an abstract superconformal field theory. The latter is supposedly related to the strong-coupling dynamics of $N_c$ coincident M5 branes, dual, in the large-$N_c$ limit, to the bulk M-theory compactified on AdS$_7 \\times$S$_4$. An interpretation of extrema"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0107084","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/hep-th/0107084/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":"hep-th/0107084","created_at":"2026-07-04T17:21:05.988141+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0107084v2","created_at":"2026-07-04T17:21:05.988141+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0107084","created_at":"2026-07-04T17:21:05.988141+00:00"},{"alias_kind":"pith_short_12","alias_value":"VWNQJEHQAWOS","created_at":"2026-07-04T17:21:05.988141+00:00"},{"alias_kind":"pith_short_16","alias_value":"VWNQJEHQAWOSHLG7","created_at":"2026-07-04T17:21:05.988141+00:00"},{"alias_kind":"pith_short_8","alias_value":"VWNQJEHQ","created_at":"2026-07-04T17:21:05.988141+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS","json":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS.json","graph_json":"https://pith.science/api/pith-number/VWNQJEHQAWOSHLG76HNL73Z6MS/graph.json","events_json":"https://pith.science/api/pith-number/VWNQJEHQAWOSHLG76HNL73Z6MS/events.json","paper":"https://pith.science/paper/VWNQJEHQ"},"agent_actions":{"view_html":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS","download_json":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS.json","view_paper":"https://pith.science/paper/VWNQJEHQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0107084&json=true","fetch_graph":"https://pith.science/api/pith-number/VWNQJEHQAWOSHLG76HNL73Z6MS/graph.json","fetch_events":"https://pith.science/api/pith-number/VWNQJEHQAWOSHLG76HNL73Z6MS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS/action/storage_attestation","attest_author":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS/action/author_attestation","sign_citation":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS/action/citation_signature","submit_replication":"https://pith.science/pith/VWNQJEHQAWOSHLG76HNL73Z6MS/action/replication_record"}},"created_at":"2026-07-04T17:21:05.988141+00:00","updated_at":"2026-07-04T17:21:05.988141+00:00"}