{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:X44CPR6UWA4K5UYMSNITKDQW5E","short_pith_number":"pith:X44CPR6U","schema_version":"1.0","canonical_sha256":"bf3827c7d4b038aed30c9351350e16e911f2bd3c6399fbce52c4177e47668389","source":{"kind":"arxiv","id":"1803.07615","version":2},"attestation_state":"computed","paper":{"title":"Chaos in Continuously Monitored Quantum Systems: An Optimal Path Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Andrew N. Jordan, John Steinmetz, Philippe Lewalle","submitted_at":"2018-03-20T19:29:18Z","abstract_excerpt":"We predict that continuously monitored quantum dynamics can be chaotic. The optimal paths between past and future boundary conditions can diverge exponentially in time when there is time-dependent evolution and continuous weak monitoring. Optimal paths are defined by extremizing the global probability density to move between two boundary conditions. We investigate the onset of chaos in pure-state qubit systems with optimal paths generated by a periodic Hamiltonian. Specifically, chaotic quantum dynamics are demonstrated in a scheme where two non-commuting observables of a qubit are continuousl"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1803.07615","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-03-20T19:29:18Z","cross_cats_sorted":[],"title_canon_sha256":"975b455f02ea9d240de16ad9500a8a0cbba54d392a1dbc72528981d6d42182dc","abstract_canon_sha256":"bf75b9215b6e9df2b26375324ff8bb552a9a1cdc3a0d5c77586817e13dd543df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:08:42.917839Z","signature_b64":"Vs9BdxSaBmma+Tyg3BQTKzgyQ5pcjYuwafhB66q2vn6ZeU2FkUIiVSWbRPgZaSsA/tCjPiU1KgWlhSM5VSJ6Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf3827c7d4b038aed30c9351350e16e911f2bd3c6399fbce52c4177e47668389","last_reissued_at":"2026-05-18T00:08:42.917252Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:08:42.917252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chaos in Continuously Monitored Quantum Systems: An Optimal Path Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Andrew N. Jordan, John Steinmetz, Philippe Lewalle","submitted_at":"2018-03-20T19:29:18Z","abstract_excerpt":"We predict that continuously monitored quantum dynamics can be chaotic. The optimal paths between past and future boundary conditions can diverge exponentially in time when there is time-dependent evolution and continuous weak monitoring. Optimal paths are defined by extremizing the global probability density to move between two boundary conditions. We investigate the onset of chaos in pure-state qubit systems with optimal paths generated by a periodic Hamiltonian. Specifically, chaotic quantum dynamics are demonstrated in a scheme where two non-commuting observables of a qubit are continuousl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.07615","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":""},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1803.07615","created_at":"2026-05-18T00:08:42.917342+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.07615v2","created_at":"2026-05-18T00:08:42.917342+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.07615","created_at":"2026-05-18T00:08:42.917342+00:00"},{"alias_kind":"pith_short_12","alias_value":"X44CPR6UWA4K","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"X44CPR6UWA4K5UYM","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"X44CPR6U","created_at":"2026-05-18T12:33:01.666342+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E","json":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E.json","graph_json":"https://pith.science/api/pith-number/X44CPR6UWA4K5UYMSNITKDQW5E/graph.json","events_json":"https://pith.science/api/pith-number/X44CPR6UWA4K5UYMSNITKDQW5E/events.json","paper":"https://pith.science/paper/X44CPR6U"},"agent_actions":{"view_html":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E","download_json":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E.json","view_paper":"https://pith.science/paper/X44CPR6U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.07615&json=true","fetch_graph":"https://pith.science/api/pith-number/X44CPR6UWA4K5UYMSNITKDQW5E/graph.json","fetch_events":"https://pith.science/api/pith-number/X44CPR6UWA4K5UYMSNITKDQW5E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E/action/storage_attestation","attest_author":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E/action/author_attestation","sign_citation":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E/action/citation_signature","submit_replication":"https://pith.science/pith/X44CPR6UWA4K5UYMSNITKDQW5E/action/replication_record"}},"created_at":"2026-05-18T00:08:42.917342+00:00","updated_at":"2026-05-18T00:08:42.917342+00:00"}