{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:4XXFNCWT6QTHTPYSZ2Z7IZBCTE","short_pith_number":"pith:4XXFNCWT","schema_version":"1.0","canonical_sha256":"e5ee568ad3f42679bf12ceb3f46422990f46180723aac8815f023b1043192ad2","source":{"kind":"arxiv","id":"hep-th/0107119","version":2},"attestation_state":"computed","paper":{"title":"Giant Gravitons in Conformal Field Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Asad Naqvi, Matthew J. Strassler, Micha Berkooz, Vijay Balasubramanian","submitted_at":"2001-07-13T13:13:42Z","abstract_excerpt":"Giant gravitons in AdS_5 x S^5, and its orbifolds, have a dual field theory representation as states created by chiral primary operators. We argue that these operators are not single-trace operators in the conformal field theory, but rather are determinants and subdeterminants of scalar fields; the stringy exclusion principle applies to these operators. Evidence for this identification comes from three sources: (a) topological considerations in orbifolds, (b) computation of protected correlators using free field theory and (c) a Matrix model argument. The last argument applies to AdS_7 x S^4 a"},"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/0107119","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-07-13T13:13:42Z","cross_cats_sorted":[],"title_canon_sha256":"3968b1b35763c0349b07809733c7f6ea49a6efff4c780ea19cde1e4332f1d2ea","abstract_canon_sha256":"8fa34ce3e7064794bc36c832b0fc5c64fdfa19f8477d6a29dc3d9761b6584937"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:57.173132Z","signature_b64":"s/z/iJaiYMQkpuC6eiErhnGeJLcvi11CZtADZMmQzv/1I3V+ULB87djmHqJupEsz6BaxKtkZQlb13UmD9EN2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e5ee568ad3f42679bf12ceb3f46422990f46180723aac8815f023b1043192ad2","last_reissued_at":"2026-07-04T16:27:57.172774Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:57.172774Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Giant Gravitons in Conformal Field Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Asad Naqvi, Matthew J. Strassler, Micha Berkooz, Vijay Balasubramanian","submitted_at":"2001-07-13T13:13:42Z","abstract_excerpt":"Giant gravitons in AdS_5 x S^5, and its orbifolds, have a dual field theory representation as states created by chiral primary operators. We argue that these operators are not single-trace operators in the conformal field theory, but rather are determinants and subdeterminants of scalar fields; the stringy exclusion principle applies to these operators. Evidence for this identification comes from three sources: (a) topological considerations in orbifolds, (b) computation of protected correlators using free field theory and (c) a Matrix model argument. The last argument applies to AdS_7 x S^4 a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0107119","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/0107119/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/0107119","created_at":"2026-07-04T16:27:57.172835+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0107119v2","created_at":"2026-07-04T16:27:57.172835+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0107119","created_at":"2026-07-04T16:27:57.172835+00:00"},{"alias_kind":"pith_short_12","alias_value":"4XXFNCWT6QTH","created_at":"2026-07-04T16:27:57.172835+00:00"},{"alias_kind":"pith_short_16","alias_value":"4XXFNCWT6QTHTPYS","created_at":"2026-07-04T16:27:57.172835+00:00"},{"alias_kind":"pith_short_8","alias_value":"4XXFNCWT","created_at":"2026-07-04T16:27:57.172835+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2606.23785","citing_title":"Controlled Chaos in 4D SCFTs","ref_index":125,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21662","citing_title":"On the Universality of Probe Complexity in $\\mathcal{N}=4$ SYM","ref_index":39,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18929","citing_title":"Higher-Trace Operators and Cut Diagrammatics in the Conformal Block Expansion","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2406.19441","citing_title":"Moduli Spaces in CFT: Large Charge Operators","ref_index":77,"is_internal_anchor":true},{"citing_arxiv_id":"2508.20094","citing_title":"(Un)solvable Matrix Models for BPS Correlators","ref_index":134,"is_internal_anchor":true},{"citing_arxiv_id":"2603.28880","citing_title":"Holographic two-point functions of heavy operators revisited","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2605.02885","citing_title":"Open-Closed-Open Triality Beyond Matrix Models","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE","json":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE.json","graph_json":"https://pith.science/api/pith-number/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/graph.json","events_json":"https://pith.science/api/pith-number/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/events.json","paper":"https://pith.science/paper/4XXFNCWT"},"agent_actions":{"view_html":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE","download_json":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE.json","view_paper":"https://pith.science/paper/4XXFNCWT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0107119&json=true","fetch_graph":"https://pith.science/api/pith-number/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/graph.json","fetch_events":"https://pith.science/api/pith-number/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/action/storage_attestation","attest_author":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/action/author_attestation","sign_citation":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/action/citation_signature","submit_replication":"https://pith.science/pith/4XXFNCWT6QTHTPYSZ2Z7IZBCTE/action/replication_record"}},"created_at":"2026-07-04T16:27:57.172835+00:00","updated_at":"2026-07-04T16:27:57.172835+00:00"}