{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:H6C6G2CNIQV5OPV3PRKQCMDRIR","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":"1d95d413767e405c9f8d920a0c3b3197f71af6e512487f86f5aef9a9258981b2","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-05-30T10:38:07Z","title_canon_sha256":"8e2c615986a95c416b0357951da02ad7de1ef6e2259bdb28001b2e89d83dbec9"},"schema_version":"1.0","source":{"id":"2505.24453","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.24453","created_at":"2026-06-01T01:02:16Z"},{"alias_kind":"arxiv_version","alias_value":"2505.24453v2","created_at":"2026-06-01T01:02:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24453","created_at":"2026-06-01T01:02:16Z"},{"alias_kind":"pith_short_12","alias_value":"H6C6G2CNIQV5","created_at":"2026-06-01T01:02:16Z"},{"alias_kind":"pith_short_16","alias_value":"H6C6G2CNIQV5OPV3","created_at":"2026-06-01T01:02:16Z"},{"alias_kind":"pith_short_8","alias_value":"H6C6G2CN","created_at":"2026-06-01T01:02:16Z"}],"graph_snapshots":[{"event_id":"sha256:f6ee65b0dc98297d68ae5825a41e8340e01c098e7038cbd63d2097605738d0d0","target":"graph","created_at":"2026-06-01T01:02:16Z","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/2505.24453/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"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","authors_text":"Arul Lakshminarayan, Manju C, Uma Divakaran","cross_cats":["cond-mat.stat-mech","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-05-30T10:38:07Z","title":"Disordering a permutation symmetric system: revivals, thermalization and chaos"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24453","kind":"arxiv","version":2},"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:fd98559e4d1f6afea80ecc69205af0923333e0e638cc696fc656e7da21658b48","target":"record","created_at":"2026-06-01T01:02:16Z","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":"1d95d413767e405c9f8d920a0c3b3197f71af6e512487f86f5aef9a9258981b2","cross_cats_sorted":["cond-mat.stat-mech","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-05-30T10:38:07Z","title_canon_sha256":"8e2c615986a95c416b0357951da02ad7de1ef6e2259bdb28001b2e89d83dbec9"},"schema_version":"1.0","source":{"id":"2505.24453","kind":"arxiv","version":2}},"canonical_sha256":"3f85e3684d442bd73ebb7c55013071444685ab130b4ca033eb655f3ac13e13f8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3f85e3684d442bd73ebb7c55013071444685ab130b4ca033eb655f3ac13e13f8","first_computed_at":"2026-06-01T01:02:16.371623Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-01T01:02:16.371623Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"C1/YMh+tyL26OHeNupWfwre4Dhc3qhULoH8wq12von8Dew3m0PEA3252oVjFQp9P20WbQ8y15HhoMJnDuqnzDQ==","signature_status":"signed_v1","signed_at":"2026-06-01T01:02:16.372725Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.24453","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd98559e4d1f6afea80ecc69205af0923333e0e638cc696fc656e7da21658b48","sha256:f6ee65b0dc98297d68ae5825a41e8340e01c098e7038cbd63d2097605738d0d0"],"state_sha256":"c5b7d1366fb04a1a5f688bec36e42da7964e3db072fdc8a03a27f709a84870d6"}