{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:QVYMYAW7BM3DBTQAL6WG3BYXV7","short_pith_number":"pith:QVYMYAW7","canonical_record":{"source":{"id":"2411.19217","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-28T15:38:36Z","cross_cats_sorted":[],"title_canon_sha256":"8c0a726c54d1e73bc79c5bd9bc38053573ae72a69e1e8eb091d7786d016d23a1","abstract_canon_sha256":"c7240eb2ee8f400e6be39f0947306ad14d208581a03b98bfb669d611a1863336"},"schema_version":"1.0"},"canonical_sha256":"8570cc02df0b3630ce005fac6d8717afdc9647eb444960a355c53a66abcd41cb","source":{"kind":"arxiv","id":"2411.19217","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19217","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19217v4","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19217","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_12","alias_value":"QVYMYAW7BM3D","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_16","alias_value":"QVYMYAW7BM3DBTQA","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_8","alias_value":"QVYMYAW7","created_at":"2026-06-23T03:13:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:QVYMYAW7BM3DBTQAL6WG3BYXV7","target":"record","payload":{"canonical_record":{"source":{"id":"2411.19217","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-28T15:38:36Z","cross_cats_sorted":[],"title_canon_sha256":"8c0a726c54d1e73bc79c5bd9bc38053573ae72a69e1e8eb091d7786d016d23a1","abstract_canon_sha256":"c7240eb2ee8f400e6be39f0947306ad14d208581a03b98bfb669d611a1863336"},"schema_version":"1.0"},"canonical_sha256":"8570cc02df0b3630ce005fac6d8717afdc9647eb444960a355c53a66abcd41cb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-23T03:13:44.084496Z","signature_b64":"n7Lysvnv2h/YFcs8EHeOQPvZfMddig6y4SJZCO8MUSk3Rk+l4m9dkfLxcC3iayXDiHAcry8k7jbTplu2dSYjDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8570cc02df0b3630ce005fac6d8717afdc9647eb444960a355c53a66abcd41cb","last_reissued_at":"2026-06-23T03:13:44.083948Z","signature_status":"signed_v1","first_computed_at":"2026-06-23T03:13:44.083948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.19217","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":"2026-06-23T03:13:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AWyMr5gxcsNIAm4Jv2aQCS0lz8/LBMj594O6VmWB/P7mewAwVE8xMgH3K5CvXA9v766g1AQatJP5R9q2vq77Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T20:14:53.371301Z"},"content_sha256":"c30d3e530e1199458a7ca805890b678fed8c1b608f4fb895f022dd14699238e9","schema_version":"1.0","event_id":"sha256:c30d3e530e1199458a7ca805890b678fed8c1b608f4fb895f022dd14699238e9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:QVYMYAW7BM3DBTQAL6WG3BYXV7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Revisiting the Symmetries of Galilean Electrodynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrea Fontanella, Juan Miguel Nieto Garc\\'ia","submitted_at":"2024-11-28T15:38:36Z","abstract_excerpt":"We determine the symmetries of four different theories: I) Galilean Electrodynamics (GED), II) GED coupled to 5 free static scalar fields, III) Galilean Yang-Mills (GYM), and IV) GYM coupled to 5 interacting scalar fields. We correct some old results in the literature, by finding that the symmetries of GED in a spacetime of generic dimension $d+1$ is always infinite dimensional, and in $3+1$ they correspond to the conformal Milne algebra extended by a spatial dilatation generator, which we call $D_x$. Finally, we comment on how these results fit into the framework of the non-relativistic AdS$_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19217","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/2411.19217/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":"2026-06-23T03:13:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"esxQb4AoEPsb0iJ7SGQIJOFfXLCHPUkMdTaEPWPnMCp6iol+ur4o7GuD1jwJ3gireVXFXfIcnHpdtyZRVSFKCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T20:14:53.371689Z"},"content_sha256":"e7cf9682ae9317e650f23f5b365343c2c4ddd6d3bd4043958677f76c85604719","schema_version":"1.0","event_id":"sha256:e7cf9682ae9317e650f23f5b365343c2c4ddd6d3bd4043958677f76c85604719"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/bundle.json","state_url":"https://pith.science/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/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":"2026-06-27T20:14:53Z","links":{"resolver":"https://pith.science/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7","bundle":"https://pith.science/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/bundle.json","state":"https://pith.science/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QVYMYAW7BM3DBTQAL6WG3BYXV7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:QVYMYAW7BM3DBTQAL6WG3BYXV7","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":"c7240eb2ee8f400e6be39f0947306ad14d208581a03b98bfb669d611a1863336","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-28T15:38:36Z","title_canon_sha256":"8c0a726c54d1e73bc79c5bd9bc38053573ae72a69e1e8eb091d7786d016d23a1"},"schema_version":"1.0","source":{"id":"2411.19217","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19217","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19217v4","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19217","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_12","alias_value":"QVYMYAW7BM3D","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_16","alias_value":"QVYMYAW7BM3DBTQA","created_at":"2026-06-23T03:13:44Z"},{"alias_kind":"pith_short_8","alias_value":"QVYMYAW7","created_at":"2026-06-23T03:13:44Z"}],"graph_snapshots":[{"event_id":"sha256:e7cf9682ae9317e650f23f5b365343c2c4ddd6d3bd4043958677f76c85604719","target":"graph","created_at":"2026-06-23T03:13:44Z","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/2411.19217/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We determine the symmetries of four different theories: I) Galilean Electrodynamics (GED), II) GED coupled to 5 free static scalar fields, III) Galilean Yang-Mills (GYM), and IV) GYM coupled to 5 interacting scalar fields. We correct some old results in the literature, by finding that the symmetries of GED in a spacetime of generic dimension $d+1$ is always infinite dimensional, and in $3+1$ they correspond to the conformal Milne algebra extended by a spatial dilatation generator, which we call $D_x$. Finally, we comment on how these results fit into the framework of the non-relativistic AdS$_","authors_text":"Andrea Fontanella, Juan Miguel Nieto Garc\\'ia","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-28T15:38:36Z","title":"Revisiting the Symmetries of Galilean Electrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19217","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:c30d3e530e1199458a7ca805890b678fed8c1b608f4fb895f022dd14699238e9","target":"record","created_at":"2026-06-23T03:13:44Z","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":"c7240eb2ee8f400e6be39f0947306ad14d208581a03b98bfb669d611a1863336","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-11-28T15:38:36Z","title_canon_sha256":"8c0a726c54d1e73bc79c5bd9bc38053573ae72a69e1e8eb091d7786d016d23a1"},"schema_version":"1.0","source":{"id":"2411.19217","kind":"arxiv","version":4}},"canonical_sha256":"8570cc02df0b3630ce005fac6d8717afdc9647eb444960a355c53a66abcd41cb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8570cc02df0b3630ce005fac6d8717afdc9647eb444960a355c53a66abcd41cb","first_computed_at":"2026-06-23T03:13:44.083948Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-23T03:13:44.083948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"n7Lysvnv2h/YFcs8EHeOQPvZfMddig6y4SJZCO8MUSk3Rk+l4m9dkfLxcC3iayXDiHAcry8k7jbTplu2dSYjDw==","signature_status":"signed_v1","signed_at":"2026-06-23T03:13:44.084496Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.19217","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c30d3e530e1199458a7ca805890b678fed8c1b608f4fb895f022dd14699238e9","sha256:e7cf9682ae9317e650f23f5b365343c2c4ddd6d3bd4043958677f76c85604719"],"state_sha256":"2f97122accd8f2e0180f3ce1b1280e639a80cd239ef5f74b7f12287e7228e4e2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PeTaVeoBAYSGe1jp9boR+3yJ4PZr00Kj6MVyGWyTMqFcTTUlfsUuzcg/64aD+JQSfU5NCMyIXpLdgjbzhQyoBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T20:14:53.373612Z","bundle_sha256":"fb20a62abe7618aacf45d2b0ef165d0a247ec002c4d8d2dff7160577e7ae67a5"}}