{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:WKWAA2LPE7BJHXB3ZEMLRERJ7S","short_pith_number":"pith:WKWAA2LP","schema_version":"1.0","canonical_sha256":"b2ac00696f27c293dc3bc918b89229fc88170447263fe641f31f93935e653189","source":{"kind":"arxiv","id":"2605.18725","version":1},"attestation_state":"computed","paper":{"title":"Signatures of Quantum Chaos in the D1D5 System","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Haoyu Zhang","submitted_at":"2026-05-18T17:51:01Z","abstract_excerpt":"We investigate the emergence of random-matrix statistics in the D1D5 CFT by studying second-order lifting matrices in low-energy near-BPS sectors. We compare the $N=3$ finite-$N$ lifting problems with the planar large-$N$ limit at fixed orbifold conformal weight and R charges. In the planar large-$N$ limit at fixed orbifold energy, mixing between single-cycle and multi-cycle states is suppressed, and the symmetry-resolved lifting spectra display Poisson-like level statistics. At finite $N$, non-planar terms restore this mixing between different cycle structures. Within the resulting symmetry-r"},"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":"2605.18725","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2026-05-18T17:51:01Z","cross_cats_sorted":[],"title_canon_sha256":"65574644f70ca505aaa247bf97f6861cf0d64540f1581e2798888dc9ffdcc085","abstract_canon_sha256":"9df006e2471d3cb5d4d7f1c969992a2d888707b5a83d7a1ddcb6795e4a463cca"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:06:17.329836Z","signature_b64":"maM0ZgCkUM1SQSTthAOjYWiyObn/AAP3pz8thwWakAjg+8FExLattUzXdKp32OYpyYQRoqyWWBMobE/+Dq+iAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b2ac00696f27c293dc3bc918b89229fc88170447263fe641f31f93935e653189","last_reissued_at":"2026-05-20T00:06:17.329008Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:06:17.329008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Signatures of Quantum Chaos in the D1D5 System","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Haoyu Zhang","submitted_at":"2026-05-18T17:51:01Z","abstract_excerpt":"We investigate the emergence of random-matrix statistics in the D1D5 CFT by studying second-order lifting matrices in low-energy near-BPS sectors. We compare the $N=3$ finite-$N$ lifting problems with the planar large-$N$ limit at fixed orbifold conformal weight and R charges. In the planar large-$N$ limit at fixed orbifold energy, mixing between single-cycle and multi-cycle states is suppressed, and the symmetry-resolved lifting spectra display Poisson-like level statistics. At finite $N$, non-planar terms restore this mixing between different cycle structures. Within the resulting symmetry-r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.18725","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/2605.18725/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"claim_evidence","ran_at":"2026-05-20T00:01:59.031435Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"503157bf86b336a504d73f00a1b538057c00cf962ae6ca869da4eef567446d7d"},"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":"2605.18725","created_at":"2026-05-20T00:06:17.329144+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.18725v1","created_at":"2026-05-20T00:06:17.329144+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.18725","created_at":"2026-05-20T00:06:17.329144+00:00"},{"alias_kind":"pith_short_12","alias_value":"WKWAA2LPE7BJ","created_at":"2026-05-20T00:06:17.329144+00:00"},{"alias_kind":"pith_short_16","alias_value":"WKWAA2LPE7BJHXB3","created_at":"2026-05-20T00:06:17.329144+00:00"},{"alias_kind":"pith_short_8","alias_value":"WKWAA2LP","created_at":"2026-05-20T00:06:17.329144+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/WKWAA2LPE7BJHXB3ZEMLRERJ7S","json":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S.json","graph_json":"https://pith.science/api/pith-number/WKWAA2LPE7BJHXB3ZEMLRERJ7S/graph.json","events_json":"https://pith.science/api/pith-number/WKWAA2LPE7BJHXB3ZEMLRERJ7S/events.json","paper":"https://pith.science/paper/WKWAA2LP"},"agent_actions":{"view_html":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S","download_json":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S.json","view_paper":"https://pith.science/paper/WKWAA2LP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.18725&json=true","fetch_graph":"https://pith.science/api/pith-number/WKWAA2LPE7BJHXB3ZEMLRERJ7S/graph.json","fetch_events":"https://pith.science/api/pith-number/WKWAA2LPE7BJHXB3ZEMLRERJ7S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S/action/storage_attestation","attest_author":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S/action/author_attestation","sign_citation":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S/action/citation_signature","submit_replication":"https://pith.science/pith/WKWAA2LPE7BJHXB3ZEMLRERJ7S/action/replication_record"}},"created_at":"2026-05-20T00:06:17.329144+00:00","updated_at":"2026-05-20T00:06:17.329144+00:00"}