{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:4Z35LGTDHCIVNIMC5S7BRBORW4","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":"aa8f221db19eab5b07d70a8dfddb2fda4937c014c218539fe68f0e382fef8e04","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-27T16:16:20Z","title_canon_sha256":"f0f76b67055abd21bf102cb4763a12dbe9b9503b969e136c358681a11e703c93"},"schema_version":"1.0","source":{"id":"2212.13536","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.13536","created_at":"2026-07-05T06:04:35Z"},{"alias_kind":"arxiv_version","alias_value":"2212.13536v2","created_at":"2026-07-05T06:04:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.13536","created_at":"2026-07-05T06:04:35Z"},{"alias_kind":"pith_short_12","alias_value":"4Z35LGTDHCIV","created_at":"2026-07-05T06:04:35Z"},{"alias_kind":"pith_short_16","alias_value":"4Z35LGTDHCIVNIMC","created_at":"2026-07-05T06:04:35Z"},{"alias_kind":"pith_short_8","alias_value":"4Z35LGTD","created_at":"2026-07-05T06:04:35Z"}],"graph_snapshots":[{"event_id":"sha256:6b27688427c76f7659208e653ef034d977b1ff67e2196ef3f32afbb93d852e21","target":"graph","created_at":"2026-07-05T06:04:35Z","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/2212.13536/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Recently, it was discovered that certain non-Hermitian systems can exhibit qualitative different properties at different system sizes, such as being gapless at small sizes and having topological edge modes at large sizes $L$. This dramatic system size sensitivity is known as the critical non-Hermitian skin effect (cNHSE), and occurs due to the competition between two or more non-Hermitian pumping channels. In this work, we rigorously develop the notion of a size-dependent generalized Brillouin zone (GBZ) in a general multi-component cNHSE model ansatz, and found that the GBZ exhibits a univers","authors_text":"Ching Hua Lee, Fang Qin, Ruizhe Shen, Ye Ma","cross_cats":["physics.optics"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-27T16:16:20Z","title":"Universal competitive spectral scaling from the critical non-Hermitian skin effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.13536","kind":"arxiv","version":2},"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":"sha256:56fe091bdfe688bcddc463407164f3a4fe624cbe711d5d06227d97f4f74ece4a","target":"record","created_at":"2026-07-05T06:04:35Z","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":"aa8f221db19eab5b07d70a8dfddb2fda4937c014c218539fe68f0e382fef8e04","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-27T16:16:20Z","title_canon_sha256":"f0f76b67055abd21bf102cb4763a12dbe9b9503b969e136c358681a11e703c93"},"schema_version":"1.0","source":{"id":"2212.13536","kind":"arxiv","version":2}},"canonical_sha256":"e677d59a63389156a182ecbe1885d1b720769f51e7317434a1d42967c18b56e0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e677d59a63389156a182ecbe1885d1b720769f51e7317434a1d42967c18b56e0","first_computed_at":"2026-07-05T06:04:35.918717Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:04:35.918717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"z1YtRbpV63Hmx4KHTC0Yvf337/hVwmtt3f/eOg1PVCSrtDViz5nmlFj4FWCasA8tAiyZT8nrc2k3YRKDut1YDw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:04:35.919242Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.13536","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:56fe091bdfe688bcddc463407164f3a4fe624cbe711d5d06227d97f4f74ece4a","sha256:6b27688427c76f7659208e653ef034d977b1ff67e2196ef3f32afbb93d852e21"],"state_sha256":"6748f131fecfb3bdaf5e0d171a50e3b053f55acc76f6404d391dff8b4c78d945"}