{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ADEWSFGKKVCLWH3DJSW5PD5ONK","short_pith_number":"pith:ADEWSFGK","schema_version":"1.0","canonical_sha256":"00c96914ca5544bb1f634cadd78fae6a9caef73661acee6a99bae28af171fd3b","source":{"kind":"arxiv","id":"2401.16591","version":1},"attestation_state":"computed","paper":{"title":"Celestial Holography Revisited II: Correlators and K\\\"all\\'en-Lehmann","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Charlotte Sleight, Lorenzo Iacobacci, Massimo Taronna","submitted_at":"2024-01-29T21:45:55Z","abstract_excerpt":"In this work we continue the investigation of the extrapolate dictionary for celestial holography recently proposed in [2301.01810], at both the perturbative and non-perturbative level. Focusing on scalar field theories, we give a complete set of Feynman rules for extrapolate celestial correlation functions and their radial reduction in the hyperbolic slicing of Minkowski space. We prove to all orders in perturbation theory that celestial correlators can be re-written in terms of corresponding Witten diagrams in EAdS which, in the hyperbolic slicing of Minkowski space, follows from the fact th"},"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":"2401.16591","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-01-29T21:45:55Z","cross_cats_sorted":[],"title_canon_sha256":"d6ac67ad2ff1fa42dbc7c833505d39ef3cfb100fbc63dbf1c45489f7edce6c8a","abstract_canon_sha256":"6ba63406032f6f7956148d4bd2ee0e4bc92b819f332b1cf0d216a434bb1be88a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:38:57.418125Z","signature_b64":"0llhU6u7qu0pSGMMHVX/2NnSfCRPx95iGVJrJduY9ANN3bwrbWYmrhlfr+zNgrBkPoMOoSj4XQ4GHYgFdApHCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00c96914ca5544bb1f634cadd78fae6a9caef73661acee6a99bae28af171fd3b","last_reissued_at":"2026-07-05T07:38:57.416661Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:38:57.416661Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Celestial Holography Revisited II: Correlators and K\\\"all\\'en-Lehmann","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Charlotte Sleight, Lorenzo Iacobacci, Massimo Taronna","submitted_at":"2024-01-29T21:45:55Z","abstract_excerpt":"In this work we continue the investigation of the extrapolate dictionary for celestial holography recently proposed in [2301.01810], at both the perturbative and non-perturbative level. Focusing on scalar field theories, we give a complete set of Feynman rules for extrapolate celestial correlation functions and their radial reduction in the hyperbolic slicing of Minkowski space. We prove to all orders in perturbation theory that celestial correlators can be re-written in terms of corresponding Witten diagrams in EAdS which, in the hyperbolic slicing of Minkowski space, follows from the fact th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.16591","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2401.16591/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":"2401.16591","created_at":"2026-07-05T07:38:57.416723+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.16591v1","created_at":"2026-07-05T07:38:57.416723+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.16591","created_at":"2026-07-05T07:38:57.416723+00:00"},{"alias_kind":"pith_short_12","alias_value":"ADEWSFGKKVCL","created_at":"2026-07-05T07:38:57.416723+00:00"},{"alias_kind":"pith_short_16","alias_value":"ADEWSFGKKVCLWH3D","created_at":"2026-07-05T07:38:57.416723+00:00"},{"alias_kind":"pith_short_8","alias_value":"ADEWSFGK","created_at":"2026-07-05T07:38:57.416723+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","ref_index":218,"is_internal_anchor":false},{"citing_arxiv_id":"2606.20433","citing_title":"Shadow Completion in Celestial OPEs","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","ref_index":225,"is_internal_anchor":false},{"citing_arxiv_id":"2605.27870","citing_title":"Revisiting boundary electromagnetic duality and edge modes","ref_index":81,"is_internal_anchor":false},{"citing_arxiv_id":"2509.04974","citing_title":"Minkowski Space holography and Radon transform","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03155","citing_title":"Flat Space Physics from AdS Actions","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK","json":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK.json","graph_json":"https://pith.science/api/pith-number/ADEWSFGKKVCLWH3DJSW5PD5ONK/graph.json","events_json":"https://pith.science/api/pith-number/ADEWSFGKKVCLWH3DJSW5PD5ONK/events.json","paper":"https://pith.science/paper/ADEWSFGK"},"agent_actions":{"view_html":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK","download_json":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK.json","view_paper":"https://pith.science/paper/ADEWSFGK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.16591&json=true","fetch_graph":"https://pith.science/api/pith-number/ADEWSFGKKVCLWH3DJSW5PD5ONK/graph.json","fetch_events":"https://pith.science/api/pith-number/ADEWSFGKKVCLWH3DJSW5PD5ONK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK/action/storage_attestation","attest_author":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK/action/author_attestation","sign_citation":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK/action/citation_signature","submit_replication":"https://pith.science/pith/ADEWSFGKKVCLWH3DJSW5PD5ONK/action/replication_record"}},"created_at":"2026-07-05T07:38:57.416723+00:00","updated_at":"2026-07-05T07:38:57.416723+00:00"}