{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:HOBFASWVJG2DMVLRVEK2IKOVYE","short_pith_number":"pith:HOBFASWV","canonical_record":{"source":{"id":"2311.00695","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-11-01T17:52:23Z","cross_cats_sorted":[],"title_canon_sha256":"5b5dd6f796fda37b57c8081e41e81082d32e946a6172075d0b33da37cd26cbc2","abstract_canon_sha256":"f58701cb09866cd429cf7d95b18bef9c609a2c3850d6efd4ac3a640653eee7c4"},"schema_version":"1.0"},"canonical_sha256":"3b82504ad549b4365571a915a429d5c114a8cc97123b5ce6a71a234427ce3869","source":{"kind":"arxiv","id":"2311.00695","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.00695","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"arxiv_version","alias_value":"2311.00695v2","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.00695","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_12","alias_value":"HOBFASWVJG2D","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_16","alias_value":"HOBFASWVJG2DMVLR","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_8","alias_value":"HOBFASWV","created_at":"2026-07-05T07:56:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:HOBFASWVJG2DMVLRVEK2IKOVYE","target":"record","payload":{"canonical_record":{"source":{"id":"2311.00695","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-11-01T17:52:23Z","cross_cats_sorted":[],"title_canon_sha256":"5b5dd6f796fda37b57c8081e41e81082d32e946a6172075d0b33da37cd26cbc2","abstract_canon_sha256":"f58701cb09866cd429cf7d95b18bef9c609a2c3850d6efd4ac3a640653eee7c4"},"schema_version":"1.0"},"canonical_sha256":"3b82504ad549b4365571a915a429d5c114a8cc97123b5ce6a71a234427ce3869","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:56:18.481899Z","signature_b64":"OqSy/r7STHp44qirudABFKaQ6/S8uWtJP8ZJQ/+2scPjKLrTkvnqiWwBfiT35RF13wUV5p3sKRYW8x10gXIRCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3b82504ad549b4365571a915a429d5c114a8cc97123b5ce6a71a234427ce3869","last_reissued_at":"2026-07-05T07:56:18.481324Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:56:18.481324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2311.00695","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":"2026-07-05T07:56:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aVN2gF9DP3YZ61XsexLlcW7tqNjJAWt1825wiyubsU/YnSVQs+BkcOOJ1npNamO0Ay+bmT6ID6qcGcw4Q/KkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T06:33:35.672019Z"},"content_sha256":"61d8b10574e4fa8980726e0e61fdf79f16fc25cb576ae485f9ccaf60d283acd3","schema_version":"1.0","event_id":"sha256:61d8b10574e4fa8980726e0e61fdf79f16fc25cb576ae485f9ccaf60d283acd3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:HOBFASWVJG2DMVLRVEK2IKOVYE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Predicting Arbitrary State Properties from Single Hamiltonian Quench Dynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Hong-Ye Hu, Zhenhuan Liu, Zihan Hao","submitted_at":"2023-11-01T17:52:23Z","abstract_excerpt":"Analog quantum simulation is an essential routine for quantum computing and plays a crucial role in studying quantum many-body physics. Typically, the quantum evolution of an analog simulator is largely determined by its physical characteristics, lacking the precise control or versatility of quantum gates. This limitation poses challenges in extracting physical properties on analog quantum simulators, an essential step of quantum simulations. To address this issue, we introduce the Hamiltonian shadow protocol, which uses a single quench Hamiltonian for estimating arbitrary state properties, el"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.00695","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/2311.00695/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":"2026-07-05T07:56:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YSnrClXpGeN4H3+Q+LPGqRsG940A9rYXR/sgrr80DVWMFETFMFEnMGkBdlaLPOfgVwwv8SBb7Dj2XTm73EsVBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T06:33:35.672719Z"},"content_sha256":"ead1a83b4598487d6910e60dcf88e67582ec015b2d2d83d60234a3d8673d5c36","schema_version":"1.0","event_id":"sha256:ead1a83b4598487d6910e60dcf88e67582ec015b2d2d83d60234a3d8673d5c36"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/bundle.json","state_url":"https://pith.science/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/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":"2026-08-05T06:33:35Z","links":{"resolver":"https://pith.science/pith/HOBFASWVJG2DMVLRVEK2IKOVYE","bundle":"https://pith.science/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/bundle.json","state":"https://pith.science/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HOBFASWVJG2DMVLRVEK2IKOVYE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:HOBFASWVJG2DMVLRVEK2IKOVYE","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":"f58701cb09866cd429cf7d95b18bef9c609a2c3850d6efd4ac3a640653eee7c4","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-11-01T17:52:23Z","title_canon_sha256":"5b5dd6f796fda37b57c8081e41e81082d32e946a6172075d0b33da37cd26cbc2"},"schema_version":"1.0","source":{"id":"2311.00695","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.00695","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"arxiv_version","alias_value":"2311.00695v2","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.00695","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_12","alias_value":"HOBFASWVJG2D","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_16","alias_value":"HOBFASWVJG2DMVLR","created_at":"2026-07-05T07:56:18Z"},{"alias_kind":"pith_short_8","alias_value":"HOBFASWV","created_at":"2026-07-05T07:56:18Z"}],"graph_snapshots":[{"event_id":"sha256:ead1a83b4598487d6910e60dcf88e67582ec015b2d2d83d60234a3d8673d5c36","target":"graph","created_at":"2026-07-05T07:56:18Z","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/2311.00695/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Analog quantum simulation is an essential routine for quantum computing and plays a crucial role in studying quantum many-body physics. Typically, the quantum evolution of an analog simulator is largely determined by its physical characteristics, lacking the precise control or versatility of quantum gates. This limitation poses challenges in extracting physical properties on analog quantum simulators, an essential step of quantum simulations. To address this issue, we introduce the Hamiltonian shadow protocol, which uses a single quench Hamiltonian for estimating arbitrary state properties, el","authors_text":"Hong-Ye Hu, Zhenhuan Liu, Zihan Hao","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-11-01T17:52:23Z","title":"Predicting Arbitrary State Properties from Single Hamiltonian Quench Dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.00695","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":"sha256:61d8b10574e4fa8980726e0e61fdf79f16fc25cb576ae485f9ccaf60d283acd3","target":"record","created_at":"2026-07-05T07:56:18Z","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":"f58701cb09866cd429cf7d95b18bef9c609a2c3850d6efd4ac3a640653eee7c4","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-11-01T17:52:23Z","title_canon_sha256":"5b5dd6f796fda37b57c8081e41e81082d32e946a6172075d0b33da37cd26cbc2"},"schema_version":"1.0","source":{"id":"2311.00695","kind":"arxiv","version":2}},"canonical_sha256":"3b82504ad549b4365571a915a429d5c114a8cc97123b5ce6a71a234427ce3869","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3b82504ad549b4365571a915a429d5c114a8cc97123b5ce6a71a234427ce3869","first_computed_at":"2026-07-05T07:56:18.481324Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:56:18.481324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OqSy/r7STHp44qirudABFKaQ6/S8uWtJP8ZJQ/+2scPjKLrTkvnqiWwBfiT35RF13wUV5p3sKRYW8x10gXIRCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:56:18.481899Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.00695","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:61d8b10574e4fa8980726e0e61fdf79f16fc25cb576ae485f9ccaf60d283acd3","sha256:ead1a83b4598487d6910e60dcf88e67582ec015b2d2d83d60234a3d8673d5c36"],"state_sha256":"3fae75ffa4cac81c6219e770c2663631555140cb61b0d64008cd52b801931f7d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K+uOy60cMdZNGtoaOM5jfNwc35XIvdbB4M+Z6u82kAMRcpvJWdIHa1/zx1+ik3Ys9Eoh1OOnnnH/istlQ7jmBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T06:33:35.679817Z","bundle_sha256":"08c6e25fbbd64c4c1bcf31d853f8b122e632194614c915b188e2de68d5edf708"}}