{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:QSW67EH42JQPVXP72IIRDOWGNZ","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":"bf289082f0fdb6c3d5b725e973576a9cd66ef9b46f8e750a5714557860db1663","cross_cats_sorted":["cond-mat.other","cond-mat.quant-gas","cond-mat.str-el","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-04-12T18:00:05Z","title_canon_sha256":"95f8911b8859cb721d414c457f322eee6d147b401824e1a5b1d8c370c7fa0560"},"schema_version":"1.0","source":{"id":"1804.04672","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.04672","created_at":"2026-05-18T00:04:58Z"},{"alias_kind":"arxiv_version","alias_value":"1804.04672v4","created_at":"2026-05-18T00:04:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.04672","created_at":"2026-05-18T00:04:58Z"},{"alias_kind":"pith_short_12","alias_value":"QSW67EH42JQP","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"QSW67EH42JQPVXP7","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"QSW67EH4","created_at":"2026-05-18T12:32:46Z"}],"graph_snapshots":[{"event_id":"sha256:70412ff96d52e01083e4e8f7ecee924513ec99c876b650ca62b0b76ca1f8a95a","target":"graph","created_at":"2026-05-18T00:04:58Z","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"},"paper":{"abstract_excerpt":"The relation between chiral edge modes and bulk Chern numbers of quantum Hall insulators is a paradigmatic example of bulk-boundary correspondence. We show that the chiral edge modes are not strictly tied to the Chern numbers defined by a non-Hermitian Bloch Hamiltonian. This breakdown of conventional bulk-boundary correspondence stems from the non-Bloch-wave behavior of eigenstates (non-Hermitian skin effect), which generates pronounced deviations of phase diagrams from the Bloch theory. We introduce non-Bloch Chern numbers that faithfully predict the numbers of chiral edge modes. The theory ","authors_text":"Fei Song, Shunyu Yao, Zhong Wang","cross_cats":["cond-mat.other","cond-mat.quant-gas","cond-mat.str-el","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-04-12T18:00:05Z","title":"Non-Hermitian Chern bands"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.04672","kind":"arxiv","version":4},"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:aa994023181a440d2ba03ce1425e102a04e33d5b03f27d3f86eda3ebc433e1f1","target":"record","created_at":"2026-05-18T00:04:58Z","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":"bf289082f0fdb6c3d5b725e973576a9cd66ef9b46f8e750a5714557860db1663","cross_cats_sorted":["cond-mat.other","cond-mat.quant-gas","cond-mat.str-el","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-04-12T18:00:05Z","title_canon_sha256":"95f8911b8859cb721d414c457f322eee6d147b401824e1a5b1d8c370c7fa0560"},"schema_version":"1.0","source":{"id":"1804.04672","kind":"arxiv","version":4}},"canonical_sha256":"84adef90fcd260faddffd21111bac66e555d87afa1cdeb0f0a17f368d8f6ace7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"84adef90fcd260faddffd21111bac66e555d87afa1cdeb0f0a17f368d8f6ace7","first_computed_at":"2026-05-18T00:04:58.955353Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:58.955353Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fV47/pDzru++UDXAzDcmH0KdCsqnR+FGrorchrgcL6TdScWa4jpWPU5tlF/zHSXkJ7GQR7Ql5qVBjGjiM0B7Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:58.955759Z","signed_message":"canonical_sha256_bytes"},"source_id":"1804.04672","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aa994023181a440d2ba03ce1425e102a04e33d5b03f27d3f86eda3ebc433e1f1","sha256:70412ff96d52e01083e4e8f7ecee924513ec99c876b650ca62b0b76ca1f8a95a"],"state_sha256":"9fbc99e5657bc0a737f3443c95df297dc060de49a7aa9ab542bbfbe5cd87eaf0"}