{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:AXEAER5ZKFU5MG3Y3WWMJA54MU","short_pith_number":"pith:AXEAER5Z","canonical_record":{"source":{"id":"2410.20372","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-27T08:27:33Z","cross_cats_sorted":[],"title_canon_sha256":"08ebff112a9b3497f16938e760b8752198e20ad4d14e223a7cc0af9f72383f54","abstract_canon_sha256":"957554c294180836daacf11a6a51c990c34cf804ac9710dbfd68efe402b96289"},"schema_version":"1.0"},"canonical_sha256":"05c80247b95169d61b78ddacc483bc652f2706cb6b2bf194297cf71270114535","source":{"kind":"arxiv","id":"2410.20372","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.20372","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"arxiv_version","alias_value":"2410.20372v2","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.20372","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_12","alias_value":"AXEAER5ZKFU5","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_16","alias_value":"AXEAER5ZKFU5MG3Y","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_8","alias_value":"AXEAER5Z","created_at":"2026-07-05T10:40:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:AXEAER5ZKFU5MG3Y3WWMJA54MU","target":"record","payload":{"canonical_record":{"source":{"id":"2410.20372","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-27T08:27:33Z","cross_cats_sorted":[],"title_canon_sha256":"08ebff112a9b3497f16938e760b8752198e20ad4d14e223a7cc0af9f72383f54","abstract_canon_sha256":"957554c294180836daacf11a6a51c990c34cf804ac9710dbfd68efe402b96289"},"schema_version":"1.0"},"canonical_sha256":"05c80247b95169d61b78ddacc483bc652f2706cb6b2bf194297cf71270114535","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:40:13.802204Z","signature_b64":"zcZ+zqxnWzmcHmw8laQ/W/lGBz71IEdnv5gTuvKQg6XD0kJwgEVoWXoQkXBl3DHnQMCg/9Pg/D/33QLup2uPBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"05c80247b95169d61b78ddacc483bc652f2706cb6b2bf194297cf71270114535","last_reissued_at":"2026-07-05T10:40:13.801730Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:40:13.801730Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2410.20372","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":"2026-07-05T10:40:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"00xbnQ8/goRGNVfpKHb2eFvPEbtk0fJuxRE7XqVworIJxIkfUGlw0QHowvh4ieSCy7O/4vFAexxlBamyyn05DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T08:12:56.639670Z"},"content_sha256":"73ae88451c48428128ec0e546cb7d4d2275ba517de07e389dad4f82dec92cc08","schema_version":"1.0","event_id":"sha256:73ae88451c48428128ec0e546cb7d4d2275ba517de07e389dad4f82dec92cc08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:AXEAER5ZKFU5MG3Y3WWMJA54MU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Carrollian propagator and amplitude in Rindler spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ang Li, Jiang Long, Jing-Long Yang","submitted_at":"2024-10-27T08:27:33Z","abstract_excerpt":"We study the three-dimensional Carrollian field theory on the Rindler horizon which is dual to a bulk massless scalar field theory in the four-dimensional Rindler wedge. The Carrollian field theory could be mapped to a two-dimensional Euclidean field theory in the transverse plane by a Fourier transform. After defining the incoming and outgoing states at the future and past Rindler horizon, respectively, we construct the boundary-to-boundary and bulk-to-boundary propagators that are consistent with the bulk Green's function in the literature. We investigate the tree-level Carrollian amplitudes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.20372","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/2410.20372/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":"2026-07-05T10:40:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T6yZubrVUaDr2l+4bga0fcBlv287En/rbVBnDxkKl4Cgdc/t02KuRNc8IW8pETO79VW7tIqKg4eUiNq+ygulBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T08:12:56.640277Z"},"content_sha256":"5409911466f9b26b3283d8a3259a7ae4ec64c163276780a38be7eda2efdac3f6","schema_version":"1.0","event_id":"sha256:5409911466f9b26b3283d8a3259a7ae4ec64c163276780a38be7eda2efdac3f6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/bundle.json","state_url":"https://pith.science/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/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":"2026-08-20T08:12:56Z","links":{"resolver":"https://pith.science/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU","bundle":"https://pith.science/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/bundle.json","state":"https://pith.science/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AXEAER5ZKFU5MG3Y3WWMJA54MU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:AXEAER5ZKFU5MG3Y3WWMJA54MU","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":"957554c294180836daacf11a6a51c990c34cf804ac9710dbfd68efe402b96289","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-27T08:27:33Z","title_canon_sha256":"08ebff112a9b3497f16938e760b8752198e20ad4d14e223a7cc0af9f72383f54"},"schema_version":"1.0","source":{"id":"2410.20372","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.20372","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"arxiv_version","alias_value":"2410.20372v2","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.20372","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_12","alias_value":"AXEAER5ZKFU5","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_16","alias_value":"AXEAER5ZKFU5MG3Y","created_at":"2026-07-05T10:40:13Z"},{"alias_kind":"pith_short_8","alias_value":"AXEAER5Z","created_at":"2026-07-05T10:40:13Z"}],"graph_snapshots":[{"event_id":"sha256:5409911466f9b26b3283d8a3259a7ae4ec64c163276780a38be7eda2efdac3f6","target":"graph","created_at":"2026-07-05T10:40:13Z","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/2410.20372/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the three-dimensional Carrollian field theory on the Rindler horizon which is dual to a bulk massless scalar field theory in the four-dimensional Rindler wedge. The Carrollian field theory could be mapped to a two-dimensional Euclidean field theory in the transverse plane by a Fourier transform. After defining the incoming and outgoing states at the future and past Rindler horizon, respectively, we construct the boundary-to-boundary and bulk-to-boundary propagators that are consistent with the bulk Green's function in the literature. We investigate the tree-level Carrollian amplitudes","authors_text":"Ang Li, Jiang Long, Jing-Long Yang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-27T08:27:33Z","title":"Carrollian propagator and amplitude in Rindler spacetime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.20372","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":"sha256:73ae88451c48428128ec0e546cb7d4d2275ba517de07e389dad4f82dec92cc08","target":"record","created_at":"2026-07-05T10:40:13Z","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":"957554c294180836daacf11a6a51c990c34cf804ac9710dbfd68efe402b96289","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-10-27T08:27:33Z","title_canon_sha256":"08ebff112a9b3497f16938e760b8752198e20ad4d14e223a7cc0af9f72383f54"},"schema_version":"1.0","source":{"id":"2410.20372","kind":"arxiv","version":2}},"canonical_sha256":"05c80247b95169d61b78ddacc483bc652f2706cb6b2bf194297cf71270114535","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"05c80247b95169d61b78ddacc483bc652f2706cb6b2bf194297cf71270114535","first_computed_at":"2026-07-05T10:40:13.801730Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:40:13.801730Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zcZ+zqxnWzmcHmw8laQ/W/lGBz71IEdnv5gTuvKQg6XD0kJwgEVoWXoQkXBl3DHnQMCg/9Pg/D/33QLup2uPBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:40:13.802204Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.20372","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:73ae88451c48428128ec0e546cb7d4d2275ba517de07e389dad4f82dec92cc08","sha256:5409911466f9b26b3283d8a3259a7ae4ec64c163276780a38be7eda2efdac3f6"],"state_sha256":"2fc569b721fd1b18800a17c86ce07e9b3531477c5ccadc1b5e581164f5710029"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0N6deXB8tRWHc7U9jtuOmObo4MlX+EQdgJw5F2vHfbC0a4Apwvyx6/yl6E90K7B01ojGmb/XVOYH9x5EXgfsAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-20T08:12:56.645351Z","bundle_sha256":"b2bdf12aa8252b173b164a8100b883471afcb8352b500dc700e626c874fb6b50"}}