{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:XIISCAT57SGZJZFJ5SFZHFQGPF","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":"0efe5309aa948fbb8f1255a385cc245a94304912f877d254a45fdea7ec64a1fe","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-02-16T18:56:05Z","title_canon_sha256":"f0fdde477521498f8df5a678ce66dc3264806ae66aa6d58af6f7710394bf1c88"},"schema_version":"1.0","source":{"id":"2302.08502","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2302.08502","created_at":"2026-07-05T07:08:05Z"},{"alias_kind":"arxiv_version","alias_value":"2302.08502v2","created_at":"2026-07-05T07:08:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.08502","created_at":"2026-07-05T07:08:05Z"},{"alias_kind":"pith_short_12","alias_value":"XIISCAT57SGZ","created_at":"2026-07-05T07:08:05Z"},{"alias_kind":"pith_short_16","alias_value":"XIISCAT57SGZJZFJ","created_at":"2026-07-05T07:08:05Z"},{"alias_kind":"pith_short_8","alias_value":"XIISCAT5","created_at":"2026-07-05T07:08:05Z"}],"graph_snapshots":[{"event_id":"sha256:e0b4de50a97100236d6517514bb291034eb856cc8e0e6ff8f2a45fc9d497b585","target":"graph","created_at":"2026-07-05T07:08:05Z","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/2302.08502/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The concept of space-evolution (or space-time duality) has emerged as a promising approach for studying quantum dynamics. The basic idea involves exchanging the roles of space and time, evolving the system using a space transfer matrix rather than the time evolution operator. The infinite-volume limit is then described by the fixed points of the latter transfer matrix, also known as influence matrices. To establish the potential of this method as a bona fide computational scheme, it is important to understand whether the influence matrices can be efficiently encoded in a classical computer. He","authors_text":"Alessandro Foligno, Bruno Bertini, Tianci Zhou","cross_cats":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-02-16T18:56:05Z","title":"Temporal Entanglement in Chaotic Quantum Circuits"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.08502","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:d128bb4a18c149c5c5d7cf07aafef4e797c58f753c4b15e7665f6b08b006f084","target":"record","created_at":"2026-07-05T07:08:05Z","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":"0efe5309aa948fbb8f1255a385cc245a94304912f877d254a45fdea7ec64a1fe","cross_cats_sorted":["cond-mat.stat-mech","hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-02-16T18:56:05Z","title_canon_sha256":"f0fdde477521498f8df5a678ce66dc3264806ae66aa6d58af6f7710394bf1c88"},"schema_version":"1.0","source":{"id":"2302.08502","kind":"arxiv","version":2}},"canonical_sha256":"ba1121027dfc8d94e4a9ec8b939606795d2d0512abebeadba73184530841dd5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ba1121027dfc8d94e4a9ec8b939606795d2d0512abebeadba73184530841dd5e","first_computed_at":"2026-07-05T07:08:05.285844Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:08:05.285844Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"URh4wExcZgSr/d8oB1FPYXvCKiXcZ2KZh7BNZEF5Bwy+8TFdjlhnUFAeGtjUSak0oYCzeX5a843VpExEh+eLAg==","signature_status":"signed_v1","signed_at":"2026-07-05T07:08:05.286374Z","signed_message":"canonical_sha256_bytes"},"source_id":"2302.08502","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d128bb4a18c149c5c5d7cf07aafef4e797c58f753c4b15e7665f6b08b006f084","sha256:e0b4de50a97100236d6517514bb291034eb856cc8e0e6ff8f2a45fc9d497b585"],"state_sha256":"0aec0b2628f878aa79abc733604d39fa4353e7d0e6ce277ad5cfd77ff8263bd3"}