{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:N3V4VXYVJ6BRF5OTZCZC35XGZR","short_pith_number":"pith:N3V4VXYV","canonical_record":{"source":{"id":"1201.6452","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-th","submitted_at":"2012-01-31T06:06:06Z","cross_cats_sorted":[],"title_canon_sha256":"13b82277cff9766707aea2f08f4aa4affdaf85a968fb6a7c83c5094baf85c010","abstract_canon_sha256":"c0ac726206d3487ff5405ade3faa18fd3ef9c590a036d036cdb300f5472d8b85"},"schema_version":"1.0"},"canonical_sha256":"6eebcadf154f8312f5d3c8b22df6e6cc68355718494775b2d88c12355c496451","source":{"kind":"arxiv","id":"1201.6452","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6452","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6452v2","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6452","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"pith_short_12","alias_value":"N3V4VXYVJ6BR","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N3V4VXYVJ6BRF5OT","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N3V4VXYV","created_at":"2026-05-18T12:27:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:N3V4VXYVJ6BRF5OTZCZC35XGZR","target":"record","payload":{"canonical_record":{"source":{"id":"1201.6452","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-th","submitted_at":"2012-01-31T06:06:06Z","cross_cats_sorted":[],"title_canon_sha256":"13b82277cff9766707aea2f08f4aa4affdaf85a968fb6a7c83c5094baf85c010","abstract_canon_sha256":"c0ac726206d3487ff5405ade3faa18fd3ef9c590a036d036cdb300f5472d8b85"},"schema_version":"1.0"},"canonical_sha256":"6eebcadf154f8312f5d3c8b22df6e6cc68355718494775b2d88c12355c496451","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:52.749467Z","signature_b64":"ELb2D0cvFEhhqY5gFsnFXrXApF3Z+o/WFV73pLkP+AdLCs8z/h9FYg+OzdfRSsMP5QcCPnkrbhrsZGfcegCeAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6eebcadf154f8312f5d3c8b22df6e6cc68355718494775b2d88c12355c496451","last_reissued_at":"2026-05-18T03:22:52.748967Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:52.748967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.6452","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:22:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"obqeabBF6aRmcmjj2TFZpZQBnkgoWL8+3ui5nUf+lYyp+UaOtcKE59VGsecDMyKJz8JFSKQuYFPTCkIllmTfBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T18:43:02.614706Z"},"content_sha256":"e199c941351397d588a30d014ad0f6689166d5efc8bdd950422f61e1171e29d1","schema_version":"1.0","event_id":"sha256:e199c941351397d588a30d014ad0f6689166d5efc8bdd950422f61e1171e29d1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:N3V4VXYVJ6BRF5OTZCZC35XGZR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Four Point Functions of the Stress Tensor and Conserved Currents in AdS_4/CFT_3","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Suvrat Raju","submitted_at":"2012-01-31T06:06:06Z","abstract_excerpt":"We compute four point functions of the stress tensor and conserved currents in AdS_4/CFT_3 using bulk perturbation theory. We work at treel level in the bulk theory, which we take to be either pure gravity or Yang Mills theory in AdS. We bypass the tedious evaluation of Witten diagrams using recently developed recursion relations for these correlators. In this approach, the four point function is obtained as the sum of residues of a rational function at easily identifiable poles. We write down an explicit formula for the four point correlator with arbitrary external helicities and momenta. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6452","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:22:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lV4N3YXzbYDsY/40RDBRcwLvWX+i1wJoYUPavhj4r+RE/sPzrSjL5XS92xaRGXlDU59yk5XI6CUAX5wZpB2XBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T18:43:02.615350Z"},"content_sha256":"1b48461642cd3c1669dd56991754455d46e50fb767029c902cd820d6e0c775cc","schema_version":"1.0","event_id":"sha256:1b48461642cd3c1669dd56991754455d46e50fb767029c902cd820d6e0c775cc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/bundle.json","state_url":"https://pith.science/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-27T18:43:02Z","links":{"resolver":"https://pith.science/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR","bundle":"https://pith.science/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/bundle.json","state":"https://pith.science/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N3V4VXYVJ6BRF5OTZCZC35XGZR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:N3V4VXYVJ6BRF5OTZCZC35XGZR","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"c0ac726206d3487ff5405ade3faa18fd3ef9c590a036d036cdb300f5472d8b85","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-th","submitted_at":"2012-01-31T06:06:06Z","title_canon_sha256":"13b82277cff9766707aea2f08f4aa4affdaf85a968fb6a7c83c5094baf85c010"},"schema_version":"1.0","source":{"id":"1201.6452","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6452","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6452v2","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6452","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"pith_short_12","alias_value":"N3V4VXYVJ6BR","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N3V4VXYVJ6BRF5OT","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N3V4VXYV","created_at":"2026-05-18T12:27:16Z"}],"graph_snapshots":[{"event_id":"sha256:1b48461642cd3c1669dd56991754455d46e50fb767029c902cd820d6e0c775cc","target":"graph","created_at":"2026-05-18T03:22:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We compute four point functions of the stress tensor and conserved currents in AdS_4/CFT_3 using bulk perturbation theory. We work at treel level in the bulk theory, which we take to be either pure gravity or Yang Mills theory in AdS. We bypass the tedious evaluation of Witten diagrams using recently developed recursion relations for these correlators. In this approach, the four point function is obtained as the sum of residues of a rational function at easily identifiable poles. We write down an explicit formula for the four point correlator with arbitrary external helicities and momenta. We ","authors_text":"Suvrat Raju","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-th","submitted_at":"2012-01-31T06:06:06Z","title":"Four Point Functions of the Stress Tensor and Conserved Currents in AdS_4/CFT_3"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6452","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:e199c941351397d588a30d014ad0f6689166d5efc8bdd950422f61e1171e29d1","target":"record","created_at":"2026-05-18T03:22:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"c0ac726206d3487ff5405ade3faa18fd3ef9c590a036d036cdb300f5472d8b85","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-th","submitted_at":"2012-01-31T06:06:06Z","title_canon_sha256":"13b82277cff9766707aea2f08f4aa4affdaf85a968fb6a7c83c5094baf85c010"},"schema_version":"1.0","source":{"id":"1201.6452","kind":"arxiv","version":2}},"canonical_sha256":"6eebcadf154f8312f5d3c8b22df6e6cc68355718494775b2d88c12355c496451","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6eebcadf154f8312f5d3c8b22df6e6cc68355718494775b2d88c12355c496451","first_computed_at":"2026-05-18T03:22:52.748967Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:22:52.748967Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ELb2D0cvFEhhqY5gFsnFXrXApF3Z+o/WFV73pLkP+AdLCs8z/h9FYg+OzdfRSsMP5QcCPnkrbhrsZGfcegCeAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:22:52.749467Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.6452","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e199c941351397d588a30d014ad0f6689166d5efc8bdd950422f61e1171e29d1","sha256:1b48461642cd3c1669dd56991754455d46e50fb767029c902cd820d6e0c775cc"],"state_sha256":"056359f038b91efd8191a9827f396c95fb6c62b3a85d687f16db693cb3cc3e9b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UA5a9LZu284+uUFK5dHbm5KO3j3/c31A3KAU1rxm5GF4oaQqw1Qb5lTXlDyhn29LjAc4u5MXO2kLo/k9wKoEBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T18:43:02.618743Z","bundle_sha256":"42d0ff93dedf25a1b1e6719c615bfba94fc8c19cf9c08eaf6b9a3f8b1a6c5f44"}}