{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:TOM4RK4C2673MN5A4FSTYN5742","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":"f950e15b2561bd9d88c5c76dc14e139e60252119c23d9ac94dea2010285ff9aa","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2024-01-02T19:00:00Z","title_canon_sha256":"9fcd48d873a311516ec2bf928c98896a4427c2b4f92b73a534c731ac59a6082f"},"schema_version":"1.0","source":{"id":"2401.01401","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2401.01401","created_at":"2026-07-05T10:20:35Z"},{"alias_kind":"arxiv_version","alias_value":"2401.01401v4","created_at":"2026-07-05T10:20:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.01401","created_at":"2026-07-05T10:20:35Z"},{"alias_kind":"pith_short_12","alias_value":"TOM4RK4C2673","created_at":"2026-07-05T10:20:35Z"},{"alias_kind":"pith_short_16","alias_value":"TOM4RK4C2673MN5A","created_at":"2026-07-05T10:20:35Z"},{"alias_kind":"pith_short_8","alias_value":"TOM4RK4C","created_at":"2026-07-05T10:20:35Z"}],"graph_snapshots":[{"event_id":"sha256:bbe74fd007edd93522ce749e323c288c056182690c522292dd661a526c662c89","target":"graph","created_at":"2026-07-05T10:20:35Z","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/2401.01401/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work, the term ``quantum chaos'' refers to spectral correlations similar to those found in the random matrix theory. Quantum chaos can be diagnosed through the analysis of level statistics using e.g.~the spectral form factor, which detects both short- and long-range level correlations. The spectral form factor corresponds to the Fourier transform of the two-point spectral correlation function and exhibits a typical slope-dip-ramp-plateau structure (aka correlation hole) when the system is chaotic. We discuss how this structure could be detected through the quench dynamics of two physic","authors_text":"Adolfo del Campo, Adway Kumar Das, Apollonas S. Matsoukas-Roubeas, Cameron Cianci, David A. Zarate-Herrada, Delmar G. A. Cabral, E. Jonathan Torres-Herrera, Lea F. Santos, Patrick Pinney, Sa\\'ul Pilatowsky-Cameo, Victor S. Batista","cross_cats":["quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2024-01-02T19:00:00Z","title":"Proposal for many-body quantum chaos detection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.01401","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":"sha256:1b02e6e7e6e2ce6f7a2decfbc1b930db842dd035ca74901afbbe2167d071d612","target":"record","created_at":"2026-07-05T10:20:35Z","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":"f950e15b2561bd9d88c5c76dc14e139e60252119c23d9ac94dea2010285ff9aa","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2024-01-02T19:00:00Z","title_canon_sha256":"9fcd48d873a311516ec2bf928c98896a4427c2b4f92b73a534c731ac59a6082f"},"schema_version":"1.0","source":{"id":"2401.01401","kind":"arxiv","version":4}},"canonical_sha256":"9b99c8ab82d7bfb637a0e1653c37bfe6a0a5dcb79aab4fedb51fb61fd0ab2a52","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9b99c8ab82d7bfb637a0e1653c37bfe6a0a5dcb79aab4fedb51fb61fd0ab2a52","first_computed_at":"2026-07-05T10:20:35.316428Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:20:35.316428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Cw1TWmuqCxC3i7/eyI4LcQm0jpt/GD1GIaHeOnKTqO4ry8OPl23QgkFilt8yHcO/gdBve9tQZ3IcBEp08n4QBw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:20:35.316935Z","signed_message":"canonical_sha256_bytes"},"source_id":"2401.01401","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1b02e6e7e6e2ce6f7a2decfbc1b930db842dd035ca74901afbbe2167d071d612","sha256:bbe74fd007edd93522ce749e323c288c056182690c522292dd661a526c662c89"],"state_sha256":"393ccb659674c4eb314b142a9959906a8776d2fcec48dff38edafbc5f7c2c7a9"}