{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:H6C6G2CNIQV5OPV3PRKQCMDRIR","short_pith_number":"pith:H6C6G2CN","schema_version":"1.0","canonical_sha256":"3f85e3684d442bd73ebb7c55013071444685ab130b4ca033eb655f3ac13e13f8","source":{"kind":"arxiv","id":"2505.24453","version":2},"attestation_state":"computed","paper":{"title":"Disordering a permutation symmetric system: revivals, thermalization and chaos","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","nlin.CD"],"primary_cat":"quant-ph","authors_text":"Arul Lakshminarayan, Manju C, Uma Divakaran","submitted_at":"2025-05-30T10:38:07Z","abstract_excerpt":"This study explores the effects of introducing a symmetry breaking disorder on the dynamics of a system invariant under particle permutation. The disorder forces quantum states, confined to the $N+1$ dimensional completely symmetric space to penetrate the exponentially large $2^N$ dimensional Hilbert space of $N$ particles. In particular, we focus on the quantum kicked top as a Floquet system of $N$ qubits, and use linear entropy, measuring single qubit entanglement, to investigate the changes in the time scales and values of saturation when disorder is introduced. In the near-integrable regim"},"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":"2505.24453","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-05-30T10:38:07Z","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"title_canon_sha256":"8e2c615986a95c416b0357951da02ad7de1ef6e2259bdb28001b2e89d83dbec9","abstract_canon_sha256":"1d95d413767e405c9f8d920a0c3b3197f71af6e512487f86f5aef9a9258981b2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-01T01:02:16.372725Z","signature_b64":"C1/YMh+tyL26OHeNupWfwre4Dhc3qhULoH8wq12von8Dew3m0PEA3252oVjFQp9P20WbQ8y15HhoMJnDuqnzDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3f85e3684d442bd73ebb7c55013071444685ab130b4ca033eb655f3ac13e13f8","last_reissued_at":"2026-06-01T01:02:16.371623Z","signature_status":"signed_v1","first_computed_at":"2026-06-01T01:02:16.371623Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Disordering a permutation symmetric system: revivals, thermalization and chaos","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","nlin.CD"],"primary_cat":"quant-ph","authors_text":"Arul Lakshminarayan, Manju C, Uma Divakaran","submitted_at":"2025-05-30T10:38:07Z","abstract_excerpt":"This study explores the effects of introducing a symmetry breaking disorder on the dynamics of a system invariant under particle permutation. The disorder forces quantum states, confined to the $N+1$ dimensional completely symmetric space to penetrate the exponentially large $2^N$ dimensional Hilbert space of $N$ particles. In particular, we focus on the quantum kicked top as a Floquet system of $N$ qubits, and use linear entropy, measuring single qubit entanglement, to investigate the changes in the time scales and values of saturation when disorder is introduced. In the near-integrable regim"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24453","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.24453/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":"2505.24453","created_at":"2026-06-01T01:02:16.371789+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.24453v2","created_at":"2026-06-01T01:02:16.371789+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24453","created_at":"2026-06-01T01:02:16.371789+00:00"},{"alias_kind":"pith_short_12","alias_value":"H6C6G2CNIQV5","created_at":"2026-06-01T01:02:16.371789+00:00"},{"alias_kind":"pith_short_16","alias_value":"H6C6G2CNIQV5OPV3","created_at":"2026-06-01T01:02:16.371789+00:00"},{"alias_kind":"pith_short_8","alias_value":"H6C6G2CN","created_at":"2026-06-01T01:02:16.371789+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/H6C6G2CNIQV5OPV3PRKQCMDRIR","json":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR.json","graph_json":"https://pith.science/api/pith-number/H6C6G2CNIQV5OPV3PRKQCMDRIR/graph.json","events_json":"https://pith.science/api/pith-number/H6C6G2CNIQV5OPV3PRKQCMDRIR/events.json","paper":"https://pith.science/paper/H6C6G2CN"},"agent_actions":{"view_html":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR","download_json":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR.json","view_paper":"https://pith.science/paper/H6C6G2CN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.24453&json=true","fetch_graph":"https://pith.science/api/pith-number/H6C6G2CNIQV5OPV3PRKQCMDRIR/graph.json","fetch_events":"https://pith.science/api/pith-number/H6C6G2CNIQV5OPV3PRKQCMDRIR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR/action/storage_attestation","attest_author":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR/action/author_attestation","sign_citation":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR/action/citation_signature","submit_replication":"https://pith.science/pith/H6C6G2CNIQV5OPV3PRKQCMDRIR/action/replication_record"}},"created_at":"2026-06-01T01:02:16.371789+00:00","updated_at":"2026-06-01T01:02:16.371789+00:00"}