{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:4Z35LGTDHCIVNIMC5S7BRBORW4","short_pith_number":"pith:4Z35LGTD","schema_version":"1.0","canonical_sha256":"e677d59a63389156a182ecbe1885d1b720769f51e7317434a1d42967c18b56e0","source":{"kind":"arxiv","id":"2212.13536","version":2},"attestation_state":"computed","paper":{"title":"Universal competitive spectral scaling from the critical non-Hermitian skin effect","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Ching Hua Lee, Fang Qin, Ruizhe Shen, Ye Ma","submitted_at":"2022-12-27T16:16:20Z","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"},"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":"2212.13536","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-27T16:16:20Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"f0f76b67055abd21bf102cb4763a12dbe9b9503b969e136c358681a11e703c93","abstract_canon_sha256":"aa8f221db19eab5b07d70a8dfddb2fda4937c014c218539fe68f0e382fef8e04"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:04:35.919242Z","signature_b64":"z1YtRbpV63Hmx4KHTC0Yvf337/hVwmtt3f/eOg1PVCSrtDViz5nmlFj4FWCasA8tAiyZT8nrc2k3YRKDut1YDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e677d59a63389156a182ecbe1885d1b720769f51e7317434a1d42967c18b56e0","last_reissued_at":"2026-07-05T06:04:35.918717Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:04:35.918717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal competitive spectral scaling from the critical non-Hermitian skin effect","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Ching Hua Lee, Fang Qin, Ruizhe Shen, Ye Ma","submitted_at":"2022-12-27T16:16:20Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.13536","kind":"arxiv","version":2},"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/2212.13536/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":"2212.13536","created_at":"2026-07-05T06:04:35.918780+00:00"},{"alias_kind":"arxiv_version","alias_value":"2212.13536v2","created_at":"2026-07-05T06:04:35.918780+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.13536","created_at":"2026-07-05T06:04:35.918780+00:00"},{"alias_kind":"pith_short_12","alias_value":"4Z35LGTDHCIV","created_at":"2026-07-05T06:04:35.918780+00:00"},{"alias_kind":"pith_short_16","alias_value":"4Z35LGTDHCIVNIMC","created_at":"2026-07-05T06:04:35.918780+00:00"},{"alias_kind":"pith_short_8","alias_value":"4Z35LGTD","created_at":"2026-07-05T06:04:35.918780+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.17187","citing_title":"Circuit structure-preserving error mitigation for High-Fidelity Quantum Simulations","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4","json":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4.json","graph_json":"https://pith.science/api/pith-number/4Z35LGTDHCIVNIMC5S7BRBORW4/graph.json","events_json":"https://pith.science/api/pith-number/4Z35LGTDHCIVNIMC5S7BRBORW4/events.json","paper":"https://pith.science/paper/4Z35LGTD"},"agent_actions":{"view_html":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4","download_json":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4.json","view_paper":"https://pith.science/paper/4Z35LGTD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2212.13536&json=true","fetch_graph":"https://pith.science/api/pith-number/4Z35LGTDHCIVNIMC5S7BRBORW4/graph.json","fetch_events":"https://pith.science/api/pith-number/4Z35LGTDHCIVNIMC5S7BRBORW4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4/action/storage_attestation","attest_author":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4/action/author_attestation","sign_citation":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4/action/citation_signature","submit_replication":"https://pith.science/pith/4Z35LGTDHCIVNIMC5S7BRBORW4/action/replication_record"}},"created_at":"2026-07-05T06:04:35.918780+00:00","updated_at":"2026-07-05T06:04:35.918780+00:00"}