{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:52HOKFCY7USKGJZY7GZDRBXKX3","short_pith_number":"pith:52HOKFCY","canonical_record":{"source":{"id":"2404.12158","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-04-18T13:05:22Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"7e67baf24a91b7293b1ee6957ed593eefd29c635c57aef8e571665fd059e2990","abstract_canon_sha256":"20a1805dc149fc7522bc13c82cc09e9a9d52ee10846ad3e9af9309a03b077c79"},"schema_version":"1.0"},"canonical_sha256":"ee8ee51458fd24a32738f9b23886eabedf537334a20a160aaf0f627c9c4143b3","source":{"kind":"arxiv","id":"2404.12158","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.12158","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"arxiv_version","alias_value":"2404.12158v1","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.12158","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_12","alias_value":"52HOKFCY7USK","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_16","alias_value":"52HOKFCY7USKGJZY","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_8","alias_value":"52HOKFCY","created_at":"2026-07-05T08:09:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:52HOKFCY7USKGJZY7GZDRBXKX3","target":"record","payload":{"canonical_record":{"source":{"id":"2404.12158","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-04-18T13:05:22Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"7e67baf24a91b7293b1ee6957ed593eefd29c635c57aef8e571665fd059e2990","abstract_canon_sha256":"20a1805dc149fc7522bc13c82cc09e9a9d52ee10846ad3e9af9309a03b077c79"},"schema_version":"1.0"},"canonical_sha256":"ee8ee51458fd24a32738f9b23886eabedf537334a20a160aaf0f627c9c4143b3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:09:36.117747Z","signature_b64":"gVM0HabHZx3FlmJW+OYpZUeFz6DPYdDQt6hIR6VZWkifqplcyXA04en/3pu44j+shN4+Ylc/sXxzlycwX+kWCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee8ee51458fd24a32738f9b23886eabedf537334a20a160aaf0f627c9c4143b3","last_reissued_at":"2026-07-05T08:09:36.117289Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:09:36.117289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2404.12158","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":"2026-07-05T08:09:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eqrslQsvPBF/oGqwt+O20Q/RCAGapMFQDUyxZ/0OamHYy47AWq26KcUmQxIZhLZ3L8nNrLwbwP+QVo0q1OYwCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T14:56:59.267424Z"},"content_sha256":"37fa94e087e5a780d03ff0566e91bcab0314e9d3c9e886b7d5aec17804baa400","schema_version":"1.0","event_id":"sha256:37fa94e087e5a780d03ff0566e91bcab0314e9d3c9e886b7d5aec17804baa400"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:52HOKFCY7USKGJZY7GZDRBXKX3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Protecting gauge symmetries in the the dynamics of SU(3) lattice gauge theories","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"hep-lat","authors_text":"Emil Mathew, Indrakshi Raychowdhury","submitted_at":"2024-04-18T13:05:22Z","abstract_excerpt":"Quantum simulation of the dynamics of a lattice gauge theory demands imposing on-site constraints. Ideally, the dynamics remain confined within the physical Hilbert space, where all the states satisfy those constraints. For non-Abelian gauge theories, implementing local constraints is non-trivial, as is keeping the dynamics confined in the physical Hilbert space, considering the erroneous quantum devices. SU(3) gauge group, albeit crucial for describing the strong interaction of nature, is notorious for studying via Hamiltonian simulation. This work presents a couple of symmetry protection pro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.12158","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/2404.12158/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":"2026-07-05T08:09:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9MobgZTyAWaDGwLvO+IYLfs+dN6aLsTp0ncviIDoVqmqAEIVgQTks1xCzfBDi6mSTepMfJd0fJmqijQhbOTNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T14:56:59.267953Z"},"content_sha256":"e8e27c1d9367435cbbd1a9af5205720f477a5b0539bf5a5cc843fff9f39dbc27","schema_version":"1.0","event_id":"sha256:e8e27c1d9367435cbbd1a9af5205720f477a5b0539bf5a5cc843fff9f39dbc27"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/52HOKFCY7USKGJZY7GZDRBXKX3/bundle.json","state_url":"https://pith.science/pith/52HOKFCY7USKGJZY7GZDRBXKX3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/52HOKFCY7USKGJZY7GZDRBXKX3/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":"2026-08-11T14:56:59Z","links":{"resolver":"https://pith.science/pith/52HOKFCY7USKGJZY7GZDRBXKX3","bundle":"https://pith.science/pith/52HOKFCY7USKGJZY7GZDRBXKX3/bundle.json","state":"https://pith.science/pith/52HOKFCY7USKGJZY7GZDRBXKX3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/52HOKFCY7USKGJZY7GZDRBXKX3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:52HOKFCY7USKGJZY7GZDRBXKX3","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":"20a1805dc149fc7522bc13c82cc09e9a9d52ee10846ad3e9af9309a03b077c79","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-04-18T13:05:22Z","title_canon_sha256":"7e67baf24a91b7293b1ee6957ed593eefd29c635c57aef8e571665fd059e2990"},"schema_version":"1.0","source":{"id":"2404.12158","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.12158","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"arxiv_version","alias_value":"2404.12158v1","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.12158","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_12","alias_value":"52HOKFCY7USK","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_16","alias_value":"52HOKFCY7USKGJZY","created_at":"2026-07-05T08:09:36Z"},{"alias_kind":"pith_short_8","alias_value":"52HOKFCY","created_at":"2026-07-05T08:09:36Z"}],"graph_snapshots":[{"event_id":"sha256:e8e27c1d9367435cbbd1a9af5205720f477a5b0539bf5a5cc843fff9f39dbc27","target":"graph","created_at":"2026-07-05T08:09:36Z","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/2404.12158/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Quantum simulation of the dynamics of a lattice gauge theory demands imposing on-site constraints. Ideally, the dynamics remain confined within the physical Hilbert space, where all the states satisfy those constraints. For non-Abelian gauge theories, implementing local constraints is non-trivial, as is keeping the dynamics confined in the physical Hilbert space, considering the erroneous quantum devices. SU(3) gauge group, albeit crucial for describing the strong interaction of nature, is notorious for studying via Hamiltonian simulation. This work presents a couple of symmetry protection pro","authors_text":"Emil Mathew, Indrakshi Raychowdhury","cross_cats":["quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-04-18T13:05:22Z","title":"Protecting gauge symmetries in the the dynamics of SU(3) lattice gauge theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.12158","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":"sha256:37fa94e087e5a780d03ff0566e91bcab0314e9d3c9e886b7d5aec17804baa400","target":"record","created_at":"2026-07-05T08:09:36Z","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":"20a1805dc149fc7522bc13c82cc09e9a9d52ee10846ad3e9af9309a03b077c79","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2024-04-18T13:05:22Z","title_canon_sha256":"7e67baf24a91b7293b1ee6957ed593eefd29c635c57aef8e571665fd059e2990"},"schema_version":"1.0","source":{"id":"2404.12158","kind":"arxiv","version":1}},"canonical_sha256":"ee8ee51458fd24a32738f9b23886eabedf537334a20a160aaf0f627c9c4143b3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee8ee51458fd24a32738f9b23886eabedf537334a20a160aaf0f627c9c4143b3","first_computed_at":"2026-07-05T08:09:36.117289Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:09:36.117289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gVM0HabHZx3FlmJW+OYpZUeFz6DPYdDQt6hIR6VZWkifqplcyXA04en/3pu44j+shN4+Ylc/sXxzlycwX+kWCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:09:36.117747Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.12158","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:37fa94e087e5a780d03ff0566e91bcab0314e9d3c9e886b7d5aec17804baa400","sha256:e8e27c1d9367435cbbd1a9af5205720f477a5b0539bf5a5cc843fff9f39dbc27"],"state_sha256":"c4b8b482d2ea54fdb899b3a1c3fbcd8d503b78cc23b54fe70aa346558a692c12"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8YFyP2Ukfv98SWzp/kCASWgCjHr9mcnTz8yIsoKtHacjNcgghEIc3YU/jgEDjdpFSOJNXyCKHDNjr4V8qht5Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T14:56:59.272682Z","bundle_sha256":"a256d789fd4c1eb8f058dc2af33126ff2ff6866a06ee184d644cd7cda180b2c4"}}