{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:OFMK3I4GOWC3FZS2W2CWUNYQU2","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":"56b5e79a616feed3cfe5e06c1fc21e23d3dbb2c2f836277fe49bb6c873425f6b","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2020-08-14T17:15:38Z","title_canon_sha256":"3eeb255ed12b9fb6ab91f16ea136101ace17569d14d38784bc48f3da9ced3345"},"schema_version":"1.0","source":{"id":"2008.06470","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2008.06470","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"arxiv_version","alias_value":"2008.06470v1","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2008.06470","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_12","alias_value":"OFMK3I4GOWC3","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_16","alias_value":"OFMK3I4GOWC3FZS2","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_8","alias_value":"OFMK3I4G","created_at":"2026-07-05T01:58:56Z"}],"graph_snapshots":[{"event_id":"sha256:3266d11c5610843bd19008034d406fbd5288596d82d792fe2e5165d2a4cb61b3","target":"graph","created_at":"2026-07-05T01:58:56Z","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/2008.06470/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A hallmark of photonic transport in non-Hermitian lattices with asymmetric hopping is the robust unidirectional flow of light, which is responsible for important phenomena such as the non-Hermitian skin effect. Here we show that the same effect can be induced by stochastic fluctuations in lattices which maintain a symmetric hopping on average. We illustrate such a fluctuation-induced non-Hermitian transport by discussing stochastic funneling of light, in which light is pushed toward an interface by the stochastic-induced skin effect.","authors_text":"Stefano Longhi","cross_cats":["cond-mat.mes-hall","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2020-08-14T17:15:38Z","title":"Stochastic non-Hermitian skin effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2008.06470","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:a6a3feae9b0950f43e31f13f3ae192285ead442183101c6b9efbadc2053da223","target":"record","created_at":"2026-07-05T01:58:56Z","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":"56b5e79a616feed3cfe5e06c1fc21e23d3dbb2c2f836277fe49bb6c873425f6b","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2020-08-14T17:15:38Z","title_canon_sha256":"3eeb255ed12b9fb6ab91f16ea136101ace17569d14d38784bc48f3da9ced3345"},"schema_version":"1.0","source":{"id":"2008.06470","kind":"arxiv","version":1}},"canonical_sha256":"7158ada3867585b2e65ab6856a3710a68477e04f4ef093adb892bb7cc01eb678","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7158ada3867585b2e65ab6856a3710a68477e04f4ef093adb892bb7cc01eb678","first_computed_at":"2026-07-05T01:58:56.162130Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:58:56.162130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"D7ljvu11oqRCxYrFkOJsZzOVs5z8VwO2nB4Bj2ATXVd85jBVqu0JKVbHidB3M4HLaVB2wzk9zU45qlmPr9eFDg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:58:56.162665Z","signed_message":"canonical_sha256_bytes"},"source_id":"2008.06470","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a6a3feae9b0950f43e31f13f3ae192285ead442183101c6b9efbadc2053da223","sha256:3266d11c5610843bd19008034d406fbd5288596d82d792fe2e5165d2a4cb61b3"],"state_sha256":"0ea9524ecb50bf851b7bca78e0cfabe42e43c280b67758b2b9c81e33d100590d"}