{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:PJ3BL6SFK6U7IFIWV2WJCNWZOW","short_pith_number":"pith:PJ3BL6SF","schema_version":"1.0","canonical_sha256":"7a7615fa4557a9f41516aeac9136d9758f479a3818ab8a2145b1f9e13ea9032b","source":{"kind":"arxiv","id":"2405.01627","version":4},"attestation_state":"computed","paper":{"title":"Dynamical Freezing in Exactly Solvable Models of Driven Chaotic Quantum Dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Debanjan Chowdhury, Haoyu Guo, Rohit Mukherjee","submitted_at":"2024-05-02T18:00:01Z","abstract_excerpt":"The late-time equilibrium behavior of generic interacting models is determined by the coupled hydrodynamic equations associated with the globally conserved quantities. In the presence of an external time-dependent drive, non-integrable systems typically thermalize to an effectively infinite-temperature state, losing all memory of their initial states. However, in the presence of a large time-periodic Floquet drive, there exist special points in phase-space where the strongly interacting system develops approximate {\\it emergent} conservation laws. Here we present results for an exactly solvabl"},"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":"2405.01627","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-05-02T18:00:01Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech","hep-th"],"title_canon_sha256":"9291f3113fbe8917bcb69523bd32b30cd41d62fbf48b53708c32ddc9658164b7","abstract_canon_sha256":"0f87a1623857df480707455826b02b6f3f5eea34f708252175a774cf96df31c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:17:32.814245Z","signature_b64":"dBJc9/Y03T0Sl4dpLvRoHY5OE4JQ3aN9yg+KX8FbhZ8bp9oXy8JeEwZbWCGzRV5r6dYxUrFdgniqLStjsDBaAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a7615fa4557a9f41516aeac9136d9758f479a3818ab8a2145b1f9e13ea9032b","last_reissued_at":"2026-07-05T11:17:32.813782Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:17:32.813782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Freezing in Exactly Solvable Models of Driven Chaotic Quantum Dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Debanjan Chowdhury, Haoyu Guo, Rohit Mukherjee","submitted_at":"2024-05-02T18:00:01Z","abstract_excerpt":"The late-time equilibrium behavior of generic interacting models is determined by the coupled hydrodynamic equations associated with the globally conserved quantities. In the presence of an external time-dependent drive, non-integrable systems typically thermalize to an effectively infinite-temperature state, losing all memory of their initial states. However, in the presence of a large time-periodic Floquet drive, there exist special points in phase-space where the strongly interacting system develops approximate {\\it emergent} conservation laws. Here we present results for an exactly solvabl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.01627","kind":"arxiv","version":4},"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/2405.01627/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2405.01627","created_at":"2026-07-05T11:17:32.813839+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.01627v4","created_at":"2026-07-05T11:17:32.813839+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.01627","created_at":"2026-07-05T11:17:32.813839+00:00"},{"alias_kind":"pith_short_12","alias_value":"PJ3BL6SFK6U7","created_at":"2026-07-05T11:17:32.813839+00:00"},{"alias_kind":"pith_short_16","alias_value":"PJ3BL6SFK6U7IFIW","created_at":"2026-07-05T11:17:32.813839+00:00"},{"alias_kind":"pith_short_8","alias_value":"PJ3BL6SF","created_at":"2026-07-05T11:17:32.813839+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.07609","citing_title":"Quantum dynamics of a spin model with an extensive degeneracy","ref_index":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW","json":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW.json","graph_json":"https://pith.science/api/pith-number/PJ3BL6SFK6U7IFIWV2WJCNWZOW/graph.json","events_json":"https://pith.science/api/pith-number/PJ3BL6SFK6U7IFIWV2WJCNWZOW/events.json","paper":"https://pith.science/paper/PJ3BL6SF"},"agent_actions":{"view_html":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW","download_json":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW.json","view_paper":"https://pith.science/paper/PJ3BL6SF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.01627&json=true","fetch_graph":"https://pith.science/api/pith-number/PJ3BL6SFK6U7IFIWV2WJCNWZOW/graph.json","fetch_events":"https://pith.science/api/pith-number/PJ3BL6SFK6U7IFIWV2WJCNWZOW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW/action/storage_attestation","attest_author":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW/action/author_attestation","sign_citation":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW/action/citation_signature","submit_replication":"https://pith.science/pith/PJ3BL6SFK6U7IFIWV2WJCNWZOW/action/replication_record"}},"created_at":"2026-07-05T11:17:32.813839+00:00","updated_at":"2026-07-05T11:17:32.813839+00:00"}