{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:4BB54ELSOJFOTQGMWQIPJHWBHF","short_pith_number":"pith:4BB54ELS","canonical_record":{"source":{"id":"2204.06462","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T15:34:36Z","cross_cats_sorted":[],"title_canon_sha256":"8adde5fa47bdf24bc15c0a794bc9bbe85c26e94c6c3472b2f36e2c23f795cb26","abstract_canon_sha256":"fd780c609836ff0edfcbad03e257d5adade7e37d4b5ed5cba92cb8ba36be8533"},"schema_version":"1.0"},"canonical_sha256":"e043de1172724ae9c0ccb410f49ec1394938596ac023ac8e4b57328e788327c1","source":{"kind":"arxiv","id":"2204.06462","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.06462","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"arxiv_version","alias_value":"2204.06462v2","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.06462","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_12","alias_value":"4BB54ELSOJFO","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_16","alias_value":"4BB54ELSOJFOTQGM","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_8","alias_value":"4BB54ELS","created_at":"2026-07-05T05:07:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:4BB54ELSOJFOTQGMWQIPJHWBHF","target":"record","payload":{"canonical_record":{"source":{"id":"2204.06462","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T15:34:36Z","cross_cats_sorted":[],"title_canon_sha256":"8adde5fa47bdf24bc15c0a794bc9bbe85c26e94c6c3472b2f36e2c23f795cb26","abstract_canon_sha256":"fd780c609836ff0edfcbad03e257d5adade7e37d4b5ed5cba92cb8ba36be8533"},"schema_version":"1.0"},"canonical_sha256":"e043de1172724ae9c0ccb410f49ec1394938596ac023ac8e4b57328e788327c1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:07:41.620373Z","signature_b64":"eh4VtZ8nET3vv3yw53yW6gSM8u4aWIEyXFOn9J1YuKZxMZ+8rqcIUOvolaXs+5lFJ1WZIw5WoG1TmmpoWbf7BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e043de1172724ae9c0ccb410f49ec1394938596ac023ac8e4b57328e788327c1","last_reissued_at":"2026-07-05T05:07:41.619861Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:07:41.619861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2204.06462","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":"2026-07-05T05:07:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qgHZmwVMAbYdk5z7dk1IQmflVN8BKzaRdfc7E9pxtMFMVCiUGbNpwAh5JCteoHP7ToEViae1AP07IA6fo5TNBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T01:25:52.790568Z"},"content_sha256":"3182a8c17c012923002f0f343cfe270fd9cafece0f29ed7b9bef0d5db88c9b44","schema_version":"1.0","event_id":"sha256:3182a8c17c012923002f0f343cfe270fd9cafece0f29ed7b9bef0d5db88c9b44"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:4BB54ELSOJFOTQGMWQIPJHWBHF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Scattering Amplitude for Massive Particles in AdS","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Abhijit Gadde, Trakshu Sharma","submitted_at":"2022-04-13T15:34:36Z","abstract_excerpt":"In this paper, we propose a conformally covariant momentum space representation of CFT correlation functions. We call it the AdS S-matrix. This representation has the property that it reduces to the S-matrix in the flat space limit. The flat space limit in question is taken by keeping all the particle masses fixed as the operator conformal dimensions go to infinity along with the AdS radius $\\mathtt{R}$. We give Feynman-like rules to compute the AdS S-matrix in $1/ \\mathtt{R}$ perturbation theory. Moreover, we relate it to the Mellin space representation of the conformal correlators in $1/ \\ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.06462","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/2204.06462/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:07:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Qk4sWXJ2/C5FYi+812uSpxbmhkdSCzVMlwOib1Jt8Kmg7ZB9fLA84XRicHJDRdmrn6OZ5qma82z96Z5AQCMxAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T01:25:52.791107Z"},"content_sha256":"95cf3f6ede21921b4d447c00a68b4f67b4f3df1ff0a551024dd190078037eb47","schema_version":"1.0","event_id":"sha256:95cf3f6ede21921b4d447c00a68b4f67b4f3df1ff0a551024dd190078037eb47"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/bundle.json","state_url":"https://pith.science/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/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":"2026-08-04T01:25:52Z","links":{"resolver":"https://pith.science/pith/4BB54ELSOJFOTQGMWQIPJHWBHF","bundle":"https://pith.science/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/bundle.json","state":"https://pith.science/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4BB54ELSOJFOTQGMWQIPJHWBHF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:4BB54ELSOJFOTQGMWQIPJHWBHF","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":"fd780c609836ff0edfcbad03e257d5adade7e37d4b5ed5cba92cb8ba36be8533","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T15:34:36Z","title_canon_sha256":"8adde5fa47bdf24bc15c0a794bc9bbe85c26e94c6c3472b2f36e2c23f795cb26"},"schema_version":"1.0","source":{"id":"2204.06462","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.06462","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"arxiv_version","alias_value":"2204.06462v2","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.06462","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_12","alias_value":"4BB54ELSOJFO","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_16","alias_value":"4BB54ELSOJFOTQGM","created_at":"2026-07-05T05:07:41Z"},{"alias_kind":"pith_short_8","alias_value":"4BB54ELS","created_at":"2026-07-05T05:07:41Z"}],"graph_snapshots":[{"event_id":"sha256:95cf3f6ede21921b4d447c00a68b4f67b4f3df1ff0a551024dd190078037eb47","target":"graph","created_at":"2026-07-05T05:07:41Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2204.06462/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper, we propose a conformally covariant momentum space representation of CFT correlation functions. We call it the AdS S-matrix. This representation has the property that it reduces to the S-matrix in the flat space limit. The flat space limit in question is taken by keeping all the particle masses fixed as the operator conformal dimensions go to infinity along with the AdS radius $\\mathtt{R}$. We give Feynman-like rules to compute the AdS S-matrix in $1/ \\mathtt{R}$ perturbation theory. Moreover, we relate it to the Mellin space representation of the conformal correlators in $1/ \\ma","authors_text":"Abhijit Gadde, Trakshu Sharma","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T15:34:36Z","title":"A Scattering Amplitude for Massive Particles in AdS"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.06462","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":"sha256:3182a8c17c012923002f0f343cfe270fd9cafece0f29ed7b9bef0d5db88c9b44","target":"record","created_at":"2026-07-05T05:07:41Z","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":"fd780c609836ff0edfcbad03e257d5adade7e37d4b5ed5cba92cb8ba36be8533","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T15:34:36Z","title_canon_sha256":"8adde5fa47bdf24bc15c0a794bc9bbe85c26e94c6c3472b2f36e2c23f795cb26"},"schema_version":"1.0","source":{"id":"2204.06462","kind":"arxiv","version":2}},"canonical_sha256":"e043de1172724ae9c0ccb410f49ec1394938596ac023ac8e4b57328e788327c1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e043de1172724ae9c0ccb410f49ec1394938596ac023ac8e4b57328e788327c1","first_computed_at":"2026-07-05T05:07:41.619861Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:07:41.619861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eh4VtZ8nET3vv3yw53yW6gSM8u4aWIEyXFOn9J1YuKZxMZ+8rqcIUOvolaXs+5lFJ1WZIw5WoG1TmmpoWbf7BA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:07:41.620373Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.06462","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3182a8c17c012923002f0f343cfe270fd9cafece0f29ed7b9bef0d5db88c9b44","sha256:95cf3f6ede21921b4d447c00a68b4f67b4f3df1ff0a551024dd190078037eb47"],"state_sha256":"a10794a0b4bf4827ca93e5a0766c18347a5d7a39db2b55d7fdd1a68ad33e5bfb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HX+wmRwmaf1VRMMr5WC/cXruU6G5lljhNcN4K9f36gg8t7nZUHAOByTOr4AvXP9GGFDt1ynpEtpYeQixpNpfBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T01:25:52.796162Z","bundle_sha256":"9ab070455892501110624d67a13d8579852887912a552b1a706868b2d4bf4389"}}