{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:6IFVOBFTPOVODK7EVX3M64D2S2","short_pith_number":"pith:6IFVOBFT","canonical_record":{"source":{"id":"2606.25803","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T13:19:08Z","cross_cats_sorted":[],"title_canon_sha256":"27af1123d0f8a64f69f30c8d96f3ce8a1f46276e9bb672fa5d3726cb3e339ca4","abstract_canon_sha256":"5ef6fec45d854d3deba9dcee7d857916f210a790f9090c64fb65a8b6a7e8a06e"},"schema_version":"1.0"},"canonical_sha256":"f20b5704b37baae1abe4adf6cf707a96b1fd85d8963bf7cd255a8397b703cd65","source":{"kind":"arxiv","id":"2606.25803","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.25803","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2606.25803v1","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.25803","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"6IFVOBFTPOVO","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"6IFVOBFTPOVODK7E","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"6IFVOBFT","created_at":"2026-06-25T01:18:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:6IFVOBFTPOVODK7EVX3M64D2S2","target":"record","payload":{"canonical_record":{"source":{"id":"2606.25803","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T13:19:08Z","cross_cats_sorted":[],"title_canon_sha256":"27af1123d0f8a64f69f30c8d96f3ce8a1f46276e9bb672fa5d3726cb3e339ca4","abstract_canon_sha256":"5ef6fec45d854d3deba9dcee7d857916f210a790f9090c64fb65a8b6a7e8a06e"},"schema_version":"1.0"},"canonical_sha256":"f20b5704b37baae1abe4adf6cf707a96b1fd85d8963bf7cd255a8397b703cd65","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-25T01:18:39.869410Z","signature_b64":"kGjjy/JUjuOhPbVUZDJnUnhgGVNls4Fb47kuak3gryV+C18zRsbFZNruw/tUksl1M2MIGUfnt8YrVdf28GdyDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f20b5704b37baae1abe4adf6cf707a96b1fd85d8963bf7cd255a8397b703cd65","last_reissued_at":"2026-06-25T01:18:39.868929Z","signature_status":"signed_v1","first_computed_at":"2026-06-25T01:18:39.868929Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2606.25803","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-25T01:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JrXFP39+97NTbLA7ArE+NOcqrKlSj7+c3nticfPVFH1uBzkST5RV2UAhuBuQ5ZFA4KLobIktVkmPtg5FJoJQBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T20:08:12.646464Z"},"content_sha256":"31cbc88a91966b0b757286ea5810a7a746568ec677da3db0b24fadd53768adb7","schema_version":"1.0","event_id":"sha256:31cbc88a91966b0b757286ea5810a7a746568ec677da3db0b24fadd53768adb7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:6IFVOBFTPOVODK7EVX3M64D2S2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Massive fields in 3D Minkowski space and boundary correlators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sudipta Dutta","submitted_at":"2026-06-24T13:19:08Z","abstract_excerpt":"A codimension-one Carrollian CFT on null infinity has been proposed as the putative dual description of asymptotically flat spacetimes and has so far been successful in describing the massless S-matrices in one higher dimension. In this work, we investigate the current proposal of Carrollian holography to include the massive fields in the bulk. We discover a broader class of correlation functions in two-dimensional Carrollian CFTs and show that they encode massive scattering amplitudes in three-dimensional Minkowski spacetime. We also construct a bulk-to-boundary propagator that generalizes th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.25803","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/2606.25803/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":"2026-06-25T01:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HWP9/HPAa0DArTMlXKDiJldJuIos8pNzD7ETZNH+ZvI2vcg/7XX+B25kM4CHXHSrbNF2GtYcXeoMRf5jjdeXAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T20:08:12.646834Z"},"content_sha256":"b456c02c1f4cfc1c9644ef28ce27b2f5eaef7d1370c558f959f3105b0212d372","schema_version":"1.0","event_id":"sha256:b456c02c1f4cfc1c9644ef28ce27b2f5eaef7d1370c558f959f3105b0212d372"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6IFVOBFTPOVODK7EVX3M64D2S2/bundle.json","state_url":"https://pith.science/pith/6IFVOBFTPOVODK7EVX3M64D2S2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6IFVOBFTPOVODK7EVX3M64D2S2/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":"2026-06-27T20:08:12Z","links":{"resolver":"https://pith.science/pith/6IFVOBFTPOVODK7EVX3M64D2S2","bundle":"https://pith.science/pith/6IFVOBFTPOVODK7EVX3M64D2S2/bundle.json","state":"https://pith.science/pith/6IFVOBFTPOVODK7EVX3M64D2S2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6IFVOBFTPOVODK7EVX3M64D2S2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:6IFVOBFTPOVODK7EVX3M64D2S2","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":"5ef6fec45d854d3deba9dcee7d857916f210a790f9090c64fb65a8b6a7e8a06e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T13:19:08Z","title_canon_sha256":"27af1123d0f8a64f69f30c8d96f3ce8a1f46276e9bb672fa5d3726cb3e339ca4"},"schema_version":"1.0","source":{"id":"2606.25803","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.25803","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2606.25803v1","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.25803","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"6IFVOBFTPOVO","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"6IFVOBFTPOVODK7E","created_at":"2026-06-25T01:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"6IFVOBFT","created_at":"2026-06-25T01:18:39Z"}],"graph_snapshots":[{"event_id":"sha256:b456c02c1f4cfc1c9644ef28ce27b2f5eaef7d1370c558f959f3105b0212d372","target":"graph","created_at":"2026-06-25T01:18:39Z","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/2606.25803/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A codimension-one Carrollian CFT on null infinity has been proposed as the putative dual description of asymptotically flat spacetimes and has so far been successful in describing the massless S-matrices in one higher dimension. In this work, we investigate the current proposal of Carrollian holography to include the massive fields in the bulk. We discover a broader class of correlation functions in two-dimensional Carrollian CFTs and show that they encode massive scattering amplitudes in three-dimensional Minkowski spacetime. We also construct a bulk-to-boundary propagator that generalizes th","authors_text":"Sudipta Dutta","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T13:19:08Z","title":"Massive fields in 3D Minkowski space and boundary correlators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.25803","kind":"arxiv","version":1},"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":"sha256:31cbc88a91966b0b757286ea5810a7a746568ec677da3db0b24fadd53768adb7","target":"record","created_at":"2026-06-25T01:18:39Z","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":"5ef6fec45d854d3deba9dcee7d857916f210a790f9090c64fb65a8b6a7e8a06e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-24T13:19:08Z","title_canon_sha256":"27af1123d0f8a64f69f30c8d96f3ce8a1f46276e9bb672fa5d3726cb3e339ca4"},"schema_version":"1.0","source":{"id":"2606.25803","kind":"arxiv","version":1}},"canonical_sha256":"f20b5704b37baae1abe4adf6cf707a96b1fd85d8963bf7cd255a8397b703cd65","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f20b5704b37baae1abe4adf6cf707a96b1fd85d8963bf7cd255a8397b703cd65","first_computed_at":"2026-06-25T01:18:39.868929Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-25T01:18:39.868929Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kGjjy/JUjuOhPbVUZDJnUnhgGVNls4Fb47kuak3gryV+C18zRsbFZNruw/tUksl1M2MIGUfnt8YrVdf28GdyDA==","signature_status":"signed_v1","signed_at":"2026-06-25T01:18:39.869410Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.25803","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:31cbc88a91966b0b757286ea5810a7a746568ec677da3db0b24fadd53768adb7","sha256:b456c02c1f4cfc1c9644ef28ce27b2f5eaef7d1370c558f959f3105b0212d372"],"state_sha256":"61eda724751d1075371c78426dbd090f7952fcf6fb7bdcf352ad64fed58727b0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3jqyuLFEilIutk1u53dD+bvhhHQyTrjXNMUK5g060xxVx74utMk9pnt/GVNe1P/3+2FtN0dZyicvCnB9pn8cAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T20:08:12.648675Z","bundle_sha256":"fd8f2dd21ac057809720d25e7e60bb271fabc44e0f21f236b0473491020f2332"}}