{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZRRX25N25VCO5E2E6FLLPQBJIZ","short_pith_number":"pith:ZRRX25N2","schema_version":"1.0","canonical_sha256":"cc637d75baed44ee9344f156b7c029465c6d334a53b7d463067027057f25b8e1","source":{"kind":"arxiv","id":"1611.01888","version":1},"attestation_state":"computed","paper":{"title":"Boundary Terms and Three-Point Functions: An AdS/CFT Puzzle Resolved","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Z. Freedman, Krzysztof Pilch, Nicholas P. Warner, Silviu S. Pufu","submitted_at":"2016-11-07T04:37:22Z","abstract_excerpt":"${\\cal N} = 8$ superconformal field theories, such as the ABJM theory at Chern-Simons level $k=1$ or $2$, contain 35 scalar operators ${\\cal O}_{IJ}$ with $\\Delta=1$ in the ${\\bf 35}_v$ representation of SO(8). The 3-point correlation function of these operators is non-vanishing, and indeed can be calculated non-perturbatively in the field theory. But its AdS$_4$ gravity dual, obtained from gauged ${\\cal N}=8$ supergravity, has no cubic $A^3$ couplings in its Lagrangian, where $A^{IJ}$ is the bulk dual of ${\\cal O}_{IJ}$. So conventional Witten diagrams cannot furnish the field theory result. "},"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":"1611.01888","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-07T04:37:22Z","cross_cats_sorted":[],"title_canon_sha256":"efd223ea8b64cc2ab6933408f367d2a3407c7d99f9337d25365dbb7744b06021","abstract_canon_sha256":"31a060f51f56f9478d1c3eb1c3bae9c4c0412b3fbf2365862753528441a0e658"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:38.601740Z","signature_b64":"4Shu6+JMaf5Q5yJRNxKfZEDLH8Ofa/o1O7wENI7donDyXM0aX+Rv3PhSAevC+oScaSexZ98sg4qiJs1Ql32HCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc637d75baed44ee9344f156b7c029465c6d334a53b7d463067027057f25b8e1","last_reissued_at":"2026-05-18T00:41:38.601027Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:38.601027Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Boundary Terms and Three-Point Functions: An AdS/CFT Puzzle Resolved","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Z. Freedman, Krzysztof Pilch, Nicholas P. Warner, Silviu S. Pufu","submitted_at":"2016-11-07T04:37:22Z","abstract_excerpt":"${\\cal N} = 8$ superconformal field theories, such as the ABJM theory at Chern-Simons level $k=1$ or $2$, contain 35 scalar operators ${\\cal O}_{IJ}$ with $\\Delta=1$ in the ${\\bf 35}_v$ representation of SO(8). The 3-point correlation function of these operators is non-vanishing, and indeed can be calculated non-perturbatively in the field theory. But its AdS$_4$ gravity dual, obtained from gauged ${\\cal N}=8$ supergravity, has no cubic $A^3$ couplings in its Lagrangian, where $A^{IJ}$ is the bulk dual of ${\\cal O}_{IJ}$. So conventional Witten diagrams cannot furnish the field theory result. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.01888","kind":"arxiv","version":1},"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":"1611.01888","created_at":"2026-05-18T00:41:38.601149+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.01888v1","created_at":"2026-05-18T00:41:38.601149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.01888","created_at":"2026-05-18T00:41:38.601149+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZRRX25N25VCO","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZRRX25N25VCO5E2E","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZRRX25N2","created_at":"2026-05-18T12:30:55.937587+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.08512","citing_title":"Beyond Discontinuities: Cosmological WFCs from the Supersymmetric Orthogonal Grassmannian","ref_index":46,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ","json":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ.json","graph_json":"https://pith.science/api/pith-number/ZRRX25N25VCO5E2E6FLLPQBJIZ/graph.json","events_json":"https://pith.science/api/pith-number/ZRRX25N25VCO5E2E6FLLPQBJIZ/events.json","paper":"https://pith.science/paper/ZRRX25N2"},"agent_actions":{"view_html":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ","download_json":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ.json","view_paper":"https://pith.science/paper/ZRRX25N2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.01888&json=true","fetch_graph":"https://pith.science/api/pith-number/ZRRX25N25VCO5E2E6FLLPQBJIZ/graph.json","fetch_events":"https://pith.science/api/pith-number/ZRRX25N25VCO5E2E6FLLPQBJIZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ/action/storage_attestation","attest_author":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ/action/author_attestation","sign_citation":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ/action/citation_signature","submit_replication":"https://pith.science/pith/ZRRX25N25VCO5E2E6FLLPQBJIZ/action/replication_record"}},"created_at":"2026-05-18T00:41:38.601149+00:00","updated_at":"2026-05-18T00:41:38.601149+00:00"}