{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:UESPWPRVTFIAGJU6PDZGRSWT6F","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":"bf1656ab762f9e061ef865dba2c9f733970573c90d796185650b0e8195727a18","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2023-04-16T07:36:28Z","title_canon_sha256":"bf7c24ddafe08645ddfed8f0a6d3c8a40151cd78a4230984a49af58aae6b0fb7"},"schema_version":"1.0","source":{"id":"2304.07713","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2304.07713","created_at":"2026-07-05T10:37:20Z"},{"alias_kind":"arxiv_version","alias_value":"2304.07713v1","created_at":"2026-07-05T10:37:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.07713","created_at":"2026-07-05T10:37:20Z"},{"alias_kind":"pith_short_12","alias_value":"UESPWPRVTFIA","created_at":"2026-07-05T10:37:20Z"},{"alias_kind":"pith_short_16","alias_value":"UESPWPRVTFIAGJU6","created_at":"2026-07-05T10:37:20Z"},{"alias_kind":"pith_short_8","alias_value":"UESPWPRV","created_at":"2026-07-05T10:37:20Z"}],"graph_snapshots":[{"event_id":"sha256:5b1319e71717cb8adbadcdbaeee22849cad09d7bfb26c4270b95b54a2a158d9e","target":"graph","created_at":"2026-07-05T10:37:20Z","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/2304.07713/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Anderson localization is ubiquitous in wavy systems with strong static and uncorrelated disorder. The delicate destructive interference underlying Anderson localization is usually washed out in the presence of temporal fluctuations or aperiodic drives in the Hamiltonian, leading to delocalization and restoring transport. However, in one-dimensional lattices with off-diagonal disorder Anderson localization can persist for arbitrary time-dependent drivings that do not break a hidden conservation law originating from the chiral symmetry, leading to the dubbed 'localization without eigenstates'. H","authors_text":"Stefano Longhi","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2023-04-16T07:36:28Z","title":"Anderson localization without eigenstates in photonic quantum walks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2304.07713","kind":"arxiv","version":1},"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":"sha256:2c70c6b5880ea8df9586630736c52bf58abd9c6c00e8e28323668e6a879f02df","target":"record","created_at":"2026-07-05T10:37:20Z","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":"bf1656ab762f9e061ef865dba2c9f733970573c90d796185650b0e8195727a18","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2023-04-16T07:36:28Z","title_canon_sha256":"bf7c24ddafe08645ddfed8f0a6d3c8a40151cd78a4230984a49af58aae6b0fb7"},"schema_version":"1.0","source":{"id":"2304.07713","kind":"arxiv","version":1}},"canonical_sha256":"a124fb3e35995003269e78f268cad3f1778e481891f2a75c302479dc02b6b60b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a124fb3e35995003269e78f268cad3f1778e481891f2a75c302479dc02b6b60b","first_computed_at":"2026-07-05T10:37:20.135622Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:37:20.135622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"H8Z70O8aZuPV3ObEUgBPR/rnBFttj4dheR+vCATslRj7SQ0af5erSGm3upKV/URePXJ27HEQ+gokHWSTMIj9DQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:37:20.136129Z","signed_message":"canonical_sha256_bytes"},"source_id":"2304.07713","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2c70c6b5880ea8df9586630736c52bf58abd9c6c00e8e28323668e6a879f02df","sha256:5b1319e71717cb8adbadcdbaeee22849cad09d7bfb26c4270b95b54a2a158d9e"],"state_sha256":"ab2d1bea2c76e04d56614544166c04e2be5c7a57918b500b416eba8abe013e9a"}