{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:W6W4BL7CKDAZJNWFLTUBUISUE7","short_pith_number":"pith:W6W4BL7C","schema_version":"1.0","canonical_sha256":"b7adc0afe250c194b6c55ce81a225427e7c745d9c7c0728c4dea8538b28dd0c3","source":{"kind":"arxiv","id":"1710.03199","version":1},"attestation_state":"computed","paper":{"title":"Bounds on OPE Coefficients from Interference Effects in the Conformal Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clay Cordova, Gustavo J. Turiaci, Juan Maldacena","submitted_at":"2017-10-09T17:21:01Z","abstract_excerpt":"We apply the average null energy condition to obtain upper bounds on the three-point function coefficients of stress tensors and a scalar operator, $\\langle TT {\\cal O } \\rangle,$ in general CFTs. We also constrain the gravitational anomaly of $U(1)$ currents in four-dimensional CFTs, which are encoded in three-point functions of the form $\\langle TT J \\rangle$. In theories with a large $N$ AdS dual we translate these bounds into constraints on the coefficient of a higher derivative bulk term of the form $\\int \\phi\\hspace{.5mm} W^2 $. We speculate that these bounds also apply in de-Sitter. In "},"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":"1710.03199","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-10-09T17:21:01Z","cross_cats_sorted":[],"title_canon_sha256":"b16fc4d1562328942cdbe8efca5ffe9b1751f985b4401b0e3bab04499470e845","abstract_canon_sha256":"e1963156304c71842a517f8ee161434845820861dafcc83f692a317e248db117"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:52.361135Z","signature_b64":"aAKSSs1IUQGUapFLSsX0xIAmWZevoUP5dMRXEDCrUoShlx251Wz60QZNu6Iq0A04o1lOg8c7qkOPjr171Nu+CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7adc0afe250c194b6c55ce81a225427e7c745d9c7c0728c4dea8538b28dd0c3","last_reissued_at":"2026-05-18T00:28:52.360488Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:52.360488Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bounds on OPE Coefficients from Interference Effects in the Conformal Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clay Cordova, Gustavo J. Turiaci, Juan Maldacena","submitted_at":"2017-10-09T17:21:01Z","abstract_excerpt":"We apply the average null energy condition to obtain upper bounds on the three-point function coefficients of stress tensors and a scalar operator, $\\langle TT {\\cal O } \\rangle,$ in general CFTs. We also constrain the gravitational anomaly of $U(1)$ currents in four-dimensional CFTs, which are encoded in three-point functions of the form $\\langle TT J \\rangle$. In theories with a large $N$ AdS dual we translate these bounds into constraints on the coefficient of a higher derivative bulk term of the form $\\int \\phi\\hspace{.5mm} W^2 $. We speculate that these bounds also apply in de-Sitter. In "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.03199","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":"1710.03199","created_at":"2026-05-18T00:28:52.360596+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.03199v1","created_at":"2026-05-18T00:28:52.360596+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.03199","created_at":"2026-05-18T00:28:52.360596+00:00"},{"alias_kind":"pith_short_12","alias_value":"W6W4BL7CKDAZ","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"W6W4BL7CKDAZJNWF","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"W6W4BL7C","created_at":"2026-05-18T12:31:53.515858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.02738","citing_title":"Holographic Energy Correlators for Soft Walls","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7","json":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7.json","graph_json":"https://pith.science/api/pith-number/W6W4BL7CKDAZJNWFLTUBUISUE7/graph.json","events_json":"https://pith.science/api/pith-number/W6W4BL7CKDAZJNWFLTUBUISUE7/events.json","paper":"https://pith.science/paper/W6W4BL7C"},"agent_actions":{"view_html":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7","download_json":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7.json","view_paper":"https://pith.science/paper/W6W4BL7C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.03199&json=true","fetch_graph":"https://pith.science/api/pith-number/W6W4BL7CKDAZJNWFLTUBUISUE7/graph.json","fetch_events":"https://pith.science/api/pith-number/W6W4BL7CKDAZJNWFLTUBUISUE7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7/action/storage_attestation","attest_author":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7/action/author_attestation","sign_citation":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7/action/citation_signature","submit_replication":"https://pith.science/pith/W6W4BL7CKDAZJNWFLTUBUISUE7/action/replication_record"}},"created_at":"2026-05-18T00:28:52.360596+00:00","updated_at":"2026-05-18T00:28:52.360596+00:00"}