{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:YNFF63JI2243ZOPZBWBDOTSYVQ","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":"ec9477d46de842f2a34f01cd3013818b2b706324e630cd4821e70359c3a9246e","cross_cats_sorted":["cond-mat.str-el","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-10-23T14:23:16Z","title_canon_sha256":"d2daccc468c95c9a2d918a3b92f23a8e0627dec27df54b19c9f2c8173093a954"},"schema_version":"1.0","source":{"id":"2010.12431","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2010.12431","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"arxiv_version","alias_value":"2010.12431v1","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.12431","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_12","alias_value":"YNFF63JI2243","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_16","alias_value":"YNFF63JI2243ZOPZ","created_at":"2026-07-05T01:58:56Z"},{"alias_kind":"pith_short_8","alias_value":"YNFF63JI","created_at":"2026-07-05T01:58:56Z"}],"graph_snapshots":[{"event_id":"sha256:486220a28d754a1c12ebd3b3e2405d62bf62c7a037974796c9f3680b7bfe836f","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/2010.12431/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The non-Hermitian skin effect, i.e. eigenstate condensation at the edges in lattices with open boundaries, is an exotic manifestation of non-Hermitian systems. In Bloch theory, an effective non-Hermitian Hamiltonian is generally used to describe dissipation, which however is not norm-preserving and neglects quantum jumps. Here it is shown that in a self-consistent description of the dissipative dynamics in a one-band lattice, based on the stochastic Schr\\\"odinger equation or Lindblad master equation with a collective jump operator, the skin effect and its dynamical features are washed out. Nev","authors_text":"Stefano Longhi","cross_cats":["cond-mat.str-el","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-10-23T14:23:16Z","title":"Unraveling the Non-Hermitian Skin Effect in Dissipative Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.12431","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":"sha256:067e8f7958fa0b1ce3c5d725c023364a5d3894435785e576c90a8a8dfa3f7681","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":"ec9477d46de842f2a34f01cd3013818b2b706324e630cd4821e70359c3a9246e","cross_cats_sorted":["cond-mat.str-el","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-10-23T14:23:16Z","title_canon_sha256":"d2daccc468c95c9a2d918a3b92f23a8e0627dec27df54b19c9f2c8173093a954"},"schema_version":"1.0","source":{"id":"2010.12431","kind":"arxiv","version":1}},"canonical_sha256":"c34a5f6d28d6b9bcb9f90d82374e58ac2c9780f1e430540bd4cf4efe0ed2d198","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c34a5f6d28d6b9bcb9f90d82374e58ac2c9780f1e430540bd4cf4efe0ed2d198","first_computed_at":"2026-07-05T01:58:56.881059Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:58:56.881059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NIaWBNk7/fw+a3l7RmQlAZ+zPnkaxfXMJw5kHYMqRUAXVE+O0gEbGTj6IMPC93ddNvsWFK7aRdpcQa0dyzDKAA==","signature_status":"signed_v1","signed_at":"2026-07-05T01:58:56.881519Z","signed_message":"canonical_sha256_bytes"},"source_id":"2010.12431","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:067e8f7958fa0b1ce3c5d725c023364a5d3894435785e576c90a8a8dfa3f7681","sha256:486220a28d754a1c12ebd3b3e2405d62bf62c7a037974796c9f3680b7bfe836f"],"state_sha256":"d9742338b33891b80cc5858ab0352658bcc047ff4e6d2ad4e41ab9520541e67e"}