{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:4J6A4BJ5SXSV5FOTASZ225AJBG","short_pith_number":"pith:4J6A4BJ5","schema_version":"1.0","canonical_sha256":"e27c0e053d95e55e95d304b3ad740909baf334638188e6b052d87c3bb08f72cd","source":{"kind":"arxiv","id":"2605.24115","version":1},"attestation_state":"computed","paper":{"title":"Anderson Localization: A Floquet operator Krylov space perspective","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Aditi Mitra, Hsiu-Chung Yeh","submitted_at":"2026-05-22T18:22:47Z","abstract_excerpt":"The problem of Anderson localization, as well as the single particle localization-delocalizaton transition of the Aubry-Andr\\'e model, is studied employing operator Krylov space methods. It is shown that even when the dynamics is generated by a Hamiltonian, studying the dynamics at stroboscopic rather than continuous times has its advantages. In particular, mapping the dynamics to an effective Floquet problem results in an operator Krylov space description where quantities such as the spectral function can be computed with fewer computational resources, while a moment method exists that allows"},"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":"2605.24115","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2026-05-22T18:22:47Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"0b08d932fcfd3db873be2e702ae0d7ab223054f9f5acf0ae9acd6fcb3a5b3fdc","abstract_canon_sha256":"88fbb39cfea0b195706eac27aceca36e40e9af493711fd45272b936de0259a12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T01:02:47.108562Z","signature_b64":"4JyPq06MhEjtlVn6gZusZwOXxGn69ttJHcV160pej/JzMvQ2GH/nTbZOqCO4qMkFQGv/2yUvRXGyXVuZpb2gDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e27c0e053d95e55e95d304b3ad740909baf334638188e6b052d87c3bb08f72cd","last_reissued_at":"2026-05-26T01:02:47.107685Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T01:02:47.107685Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anderson Localization: A Floquet operator Krylov space perspective","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Aditi Mitra, Hsiu-Chung Yeh","submitted_at":"2026-05-22T18:22:47Z","abstract_excerpt":"The problem of Anderson localization, as well as the single particle localization-delocalizaton transition of the Aubry-Andr\\'e model, is studied employing operator Krylov space methods. It is shown that even when the dynamics is generated by a Hamiltonian, studying the dynamics at stroboscopic rather than continuous times has its advantages. In particular, mapping the dynamics to an effective Floquet problem results in an operator Krylov space description where quantities such as the spectral function can be computed with fewer computational resources, while a moment method exists that allows"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.24115","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/2605.24115/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":"2605.24115","created_at":"2026-05-26T01:02:47.107827+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.24115v1","created_at":"2026-05-26T01:02:47.107827+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.24115","created_at":"2026-05-26T01:02:47.107827+00:00"},{"alias_kind":"pith_short_12","alias_value":"4J6A4BJ5SXSV","created_at":"2026-05-26T01:02:47.107827+00:00"},{"alias_kind":"pith_short_16","alias_value":"4J6A4BJ5SXSV5FOT","created_at":"2026-05-26T01:02:47.107827+00:00"},{"alias_kind":"pith_short_8","alias_value":"4J6A4BJ5","created_at":"2026-05-26T01:02:47.107827+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/4J6A4BJ5SXSV5FOTASZ225AJBG","json":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG.json","graph_json":"https://pith.science/api/pith-number/4J6A4BJ5SXSV5FOTASZ225AJBG/graph.json","events_json":"https://pith.science/api/pith-number/4J6A4BJ5SXSV5FOTASZ225AJBG/events.json","paper":"https://pith.science/paper/4J6A4BJ5"},"agent_actions":{"view_html":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG","download_json":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG.json","view_paper":"https://pith.science/paper/4J6A4BJ5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.24115&json=true","fetch_graph":"https://pith.science/api/pith-number/4J6A4BJ5SXSV5FOTASZ225AJBG/graph.json","fetch_events":"https://pith.science/api/pith-number/4J6A4BJ5SXSV5FOTASZ225AJBG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG/action/storage_attestation","attest_author":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG/action/author_attestation","sign_citation":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG/action/citation_signature","submit_replication":"https://pith.science/pith/4J6A4BJ5SXSV5FOTASZ225AJBG/action/replication_record"}},"created_at":"2026-05-26T01:02:47.107827+00:00","updated_at":"2026-05-26T01:02:47.107827+00:00"}