{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:2KZVIYT67CIKQ6X2BDQ2CZH7YN","short_pith_number":"pith:2KZVIYT6","canonical_record":{"source":{"id":"2210.11585","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-th","submitted_at":"2022-10-20T20:56:25Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"9b2aebc3787ecde2aeafeb7cf58a2c92910dbf3133b150fc4bee22ca33dba0b4","abstract_canon_sha256":"9314f921b1ad28e83ae53716cd26fd3c5768a2fdc5e464c80c9a9a234696b8bb"},"schema_version":"1.0"},"canonical_sha256":"d2b354627ef890a87afa08e1a164ffc34336f9ca57f648c05e550360fe05203b","source":{"kind":"arxiv","id":"2210.11585","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.11585","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"arxiv_version","alias_value":"2210.11585v4","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.11585","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_12","alias_value":"2KZVIYT67CIK","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_16","alias_value":"2KZVIYT67CIKQ6X2","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_8","alias_value":"2KZVIYT6","created_at":"2026-07-05T09:21:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:2KZVIYT67CIKQ6X2BDQ2CZH7YN","target":"record","payload":{"canonical_record":{"source":{"id":"2210.11585","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-th","submitted_at":"2022-10-20T20:56:25Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"9b2aebc3787ecde2aeafeb7cf58a2c92910dbf3133b150fc4bee22ca33dba0b4","abstract_canon_sha256":"9314f921b1ad28e83ae53716cd26fd3c5768a2fdc5e464c80c9a9a234696b8bb"},"schema_version":"1.0"},"canonical_sha256":"d2b354627ef890a87afa08e1a164ffc34336f9ca57f648c05e550360fe05203b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:21:35.295852Z","signature_b64":"OrY9AJZnxEpyfXz8g98esqZ/VP6lt2wq/u7CAZhFPtmR24CgI1ZYrOd60LMn66Z68yvM8y71NlerUiJFpPC9CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2b354627ef890a87afa08e1a164ffc34336f9ca57f648c05e550360fe05203b","last_reissued_at":"2026-07-05T09:21:35.295467Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:21:35.295467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2210.11585","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T09:21:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hrkrHTm4PH9jNX1Fqs9J/ctPWk6hRiQX0abRhqpYRLpKZWRgPphwnWmegi0q3QoN5hHlsnE5uxNazeqUT2NhBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T00:22:02.302253Z"},"content_sha256":"f1ba9b69325b79f2e300b224c7c90d47a27d9717afdca41db3033dce5e1a7f1d","schema_version":"1.0","event_id":"sha256:f1ba9b69325b79f2e300b224c7c90d47a27d9717afdca41db3033dce5e1a7f1d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:2KZVIYT67CIKQ6X2BDQ2CZH7YN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The classical dynamics of gauge theories in the deep infrared","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Eanna E. Flanagan, Ibrahim Shehzad","submitted_at":"2022-10-20T20:56:25Z","abstract_excerpt":"Gauge and gravitational theories in asymptotically flat settings possess infinitely many conserved charges associated with large gauge transformations or diffeomorphisms that are nontrivial at infinity. To what extent do these charges constrain the scattering in these theories? It has been claimed in the literature that the constraints are trivial, due to a decoupling of hard and soft sectors for which the conserved charges constrain only the dynamics in the soft sector. We show that the argument for this decoupling fails due to the failure in infinite dimensions of a property of symplectic ge"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.11585","kind":"arxiv","version":4},"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/2210.11585/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":"2026-07-05T09:21:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xkw6VJyDOvLeDYhG1WSreLgTbx7o2tEUT5OWKikI074EMXygQlIVaRDSElfPNp1cfVbg8aJxKgMjKtlcBLQLBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T00:22:02.302763Z"},"content_sha256":"4836fc4e3f9ef1c3f821c998838cf4369f7959870b71565bcace249af659960e","schema_version":"1.0","event_id":"sha256:4836fc4e3f9ef1c3f821c998838cf4369f7959870b71565bcace249af659960e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/bundle.json","state_url":"https://pith.science/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/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":"2026-08-06T00:22:02Z","links":{"resolver":"https://pith.science/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN","bundle":"https://pith.science/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/bundle.json","state":"https://pith.science/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2KZVIYT67CIKQ6X2BDQ2CZH7YN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:2KZVIYT67CIKQ6X2BDQ2CZH7YN","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":"9314f921b1ad28e83ae53716cd26fd3c5768a2fdc5e464c80c9a9a234696b8bb","cross_cats_sorted":["gr-qc"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-th","submitted_at":"2022-10-20T20:56:25Z","title_canon_sha256":"9b2aebc3787ecde2aeafeb7cf58a2c92910dbf3133b150fc4bee22ca33dba0b4"},"schema_version":"1.0","source":{"id":"2210.11585","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.11585","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"arxiv_version","alias_value":"2210.11585v4","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.11585","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_12","alias_value":"2KZVIYT67CIK","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_16","alias_value":"2KZVIYT67CIKQ6X2","created_at":"2026-07-05T09:21:35Z"},{"alias_kind":"pith_short_8","alias_value":"2KZVIYT6","created_at":"2026-07-05T09:21:35Z"}],"graph_snapshots":[{"event_id":"sha256:4836fc4e3f9ef1c3f821c998838cf4369f7959870b71565bcace249af659960e","target":"graph","created_at":"2026-07-05T09:21:35Z","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/2210.11585/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Gauge and gravitational theories in asymptotically flat settings possess infinitely many conserved charges associated with large gauge transformations or diffeomorphisms that are nontrivial at infinity. To what extent do these charges constrain the scattering in these theories? It has been claimed in the literature that the constraints are trivial, due to a decoupling of hard and soft sectors for which the conserved charges constrain only the dynamics in the soft sector. We show that the argument for this decoupling fails due to the failure in infinite dimensions of a property of symplectic ge","authors_text":"Eanna E. Flanagan, Ibrahim Shehzad","cross_cats":["gr-qc"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-th","submitted_at":"2022-10-20T20:56:25Z","title":"The classical dynamics of gauge theories in the deep infrared"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.11585","kind":"arxiv","version":4},"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:f1ba9b69325b79f2e300b224c7c90d47a27d9717afdca41db3033dce5e1a7f1d","target":"record","created_at":"2026-07-05T09:21:35Z","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":"9314f921b1ad28e83ae53716cd26fd3c5768a2fdc5e464c80c9a9a234696b8bb","cross_cats_sorted":["gr-qc"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-th","submitted_at":"2022-10-20T20:56:25Z","title_canon_sha256":"9b2aebc3787ecde2aeafeb7cf58a2c92910dbf3133b150fc4bee22ca33dba0b4"},"schema_version":"1.0","source":{"id":"2210.11585","kind":"arxiv","version":4}},"canonical_sha256":"d2b354627ef890a87afa08e1a164ffc34336f9ca57f648c05e550360fe05203b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d2b354627ef890a87afa08e1a164ffc34336f9ca57f648c05e550360fe05203b","first_computed_at":"2026-07-05T09:21:35.295467Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:21:35.295467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OrY9AJZnxEpyfXz8g98esqZ/VP6lt2wq/u7CAZhFPtmR24CgI1ZYrOd60LMn66Z68yvM8y71NlerUiJFpPC9CA==","signature_status":"signed_v1","signed_at":"2026-07-05T09:21:35.295852Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.11585","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f1ba9b69325b79f2e300b224c7c90d47a27d9717afdca41db3033dce5e1a7f1d","sha256:4836fc4e3f9ef1c3f821c998838cf4369f7959870b71565bcace249af659960e"],"state_sha256":"88c129b2e764b1c90b2e6fb165592c43c87dd4327b127bccc618f095aaf103dc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZQP8G6wC96QZ4CJ9is066zf2/RWfzKc6uO+5tsBdoZH2ZFyTJ2n3Alvx3TGNWWKFCMUvcBQYPwkOgjfSQlptBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T00:22:02.306850Z","bundle_sha256":"7a0cff3fc7d7d30fa09fa9769fcc1ed362df0005653236c9a25aea476228ee42"}}