{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:DFIVENO3F2QIPTOPVIADEDKE3V","short_pith_number":"pith:DFIVENO3","schema_version":"1.0","canonical_sha256":"19515235db2ea087cdcfaa00320d44dd5573d1c2e4ac0aad4eb982d6dfdc7757","source":{"kind":"arxiv","id":"2605.24510","version":1},"attestation_state":"computed","paper":{"title":"Strong Eigenstate Thermalization from Mean-Ergodic Non-chaotic Dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Avadhut V. Purohit, Harshit Sharma, Udaysinh T. Bhosale","submitted_at":"2026-05-23T10:48:29Z","abstract_excerpt":"We report an example of a many-body system, derived from the double kicked top (DKT), with non-chaotic yet mean-ergodic dynamics that displays \\textit{strong} eigenstate thermalization hypothesis (ETH) in the quantum regime. The analysis addresses a key open question: whether \\textit{strong} ETH is a quantum analog of ergodicity (or mean-ergodicity). Despite non-chaotic dynamics, the fluctuations of the diagonal matrix elements of an observable scale as $D^{-1/2}$, where $D$ denotes the Hilbert space dimension. Furthermore, the off-diagonal matrix elements show Gaussian statistics together wit"},"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":"2605.24510","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-23T10:48:29Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"a8afafc6b515fbcce7a8e3682e43dc1700800b3c9fe655d86779582ad5557982","abstract_canon_sha256":"52d2a5eb809306387e5f61ce2539e14e281b2996b80014e090468b05766f7d32"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T01:03:43.676521Z","signature_b64":"nElJVU9JvD37bo+RMBOmjr+Pa7AKuqvIjpky7rIrhENs9oILSHfEbxuYrwXalZxJq7IEjnp6n4tKXCqIMKG6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"19515235db2ea087cdcfaa00320d44dd5573d1c2e4ac0aad4eb982d6dfdc7757","last_reissued_at":"2026-05-26T01:03:43.675650Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T01:03:43.675650Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong Eigenstate Thermalization from Mean-Ergodic Non-chaotic Dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Avadhut V. Purohit, Harshit Sharma, Udaysinh T. Bhosale","submitted_at":"2026-05-23T10:48:29Z","abstract_excerpt":"We report an example of a many-body system, derived from the double kicked top (DKT), with non-chaotic yet mean-ergodic dynamics that displays \\textit{strong} eigenstate thermalization hypothesis (ETH) in the quantum regime. The analysis addresses a key open question: whether \\textit{strong} ETH is a quantum analog of ergodicity (or mean-ergodicity). Despite non-chaotic dynamics, the fluctuations of the diagonal matrix elements of an observable scale as $D^{-1/2}$, where $D$ denotes the Hilbert space dimension. Furthermore, the off-diagonal matrix elements show Gaussian statistics together wit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.24510","kind":"arxiv","version":1},"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/2605.24510/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":"2605.24510","created_at":"2026-05-26T01:03:43.675834+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.24510v1","created_at":"2026-05-26T01:03:43.675834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.24510","created_at":"2026-05-26T01:03:43.675834+00:00"},{"alias_kind":"pith_short_12","alias_value":"DFIVENO3F2QI","created_at":"2026-05-26T01:03:43.675834+00:00"},{"alias_kind":"pith_short_16","alias_value":"DFIVENO3F2QIPTOP","created_at":"2026-05-26T01:03:43.675834+00:00"},{"alias_kind":"pith_short_8","alias_value":"DFIVENO3","created_at":"2026-05-26T01:03:43.675834+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/DFIVENO3F2QIPTOPVIADEDKE3V","json":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V.json","graph_json":"https://pith.science/api/pith-number/DFIVENO3F2QIPTOPVIADEDKE3V/graph.json","events_json":"https://pith.science/api/pith-number/DFIVENO3F2QIPTOPVIADEDKE3V/events.json","paper":"https://pith.science/paper/DFIVENO3"},"agent_actions":{"view_html":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V","download_json":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V.json","view_paper":"https://pith.science/paper/DFIVENO3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.24510&json=true","fetch_graph":"https://pith.science/api/pith-number/DFIVENO3F2QIPTOPVIADEDKE3V/graph.json","fetch_events":"https://pith.science/api/pith-number/DFIVENO3F2QIPTOPVIADEDKE3V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V/action/storage_attestation","attest_author":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V/action/author_attestation","sign_citation":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V/action/citation_signature","submit_replication":"https://pith.science/pith/DFIVENO3F2QIPTOPVIADEDKE3V/action/replication_record"}},"created_at":"2026-05-26T01:03:43.675834+00:00","updated_at":"2026-05-26T01:03:43.675834+00:00"}