{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:IAAV4WLYRKYUS7IIBBPDTJ65LN","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":"a42a4b88acd7b2b8d8c6e01ec4641ccbdf949c8867a35729c538f70273958f81","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-12-26T02:58:05Z","title_canon_sha256":"09c875fe8e32a1a31e0445de6a168a845d1406aae520d0e0f083505ecc2887cf"},"schema_version":"1.0","source":{"id":"2212.12996","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.12996","created_at":"2026-07-05T07:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"2212.12996v3","created_at":"2026-07-05T07:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.12996","created_at":"2026-07-05T07:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"IAAV4WLYRKYU","created_at":"2026-07-05T07:33:48Z"},{"alias_kind":"pith_short_16","alias_value":"IAAV4WLYRKYUS7II","created_at":"2026-07-05T07:33:48Z"},{"alias_kind":"pith_short_8","alias_value":"IAAV4WLY","created_at":"2026-07-05T07:33:48Z"}],"graph_snapshots":[{"event_id":"sha256:7a12c72365ab1168673709e97308d7931b102cd907f498be1ab81fa7c6d39a73","target":"graph","created_at":"2026-07-05T07:33:48Z","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/2212.12996/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"After almost half a century of Laughlin's celebrated study of the wavefunctions of integer and fractional quantum Hall effects, there have still existed difficulties to prove whether the given wavefunction can describe gapped phase or not in general. In this work, we show the FQH states constructed from nonunitary conformal field theories (CFTs), such as Gaffiinian and Haldane-Rezayi states have a difficulty gapping out under preserving bulk-edge correspondence in the cylinder geometry. Contrary to the common understandings of the condensed matter communities, the gaplessness for these systems","authors_text":"Yoshiki Fukusumi","cross_cats":["hep-th","math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-12-26T02:58:05Z","title":"Gaplessness protected by bulk-edge correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.12996","kind":"arxiv","version":3},"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":"sha256:0569577920ce89c2a36b58dc5fc4cd5405cc70458686babf357ccede713ab281","target":"record","created_at":"2026-07-05T07:33:48Z","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":"a42a4b88acd7b2b8d8c6e01ec4641ccbdf949c8867a35729c538f70273958f81","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-12-26T02:58:05Z","title_canon_sha256":"09c875fe8e32a1a31e0445de6a168a845d1406aae520d0e0f083505ecc2887cf"},"schema_version":"1.0","source":{"id":"2212.12996","kind":"arxiv","version":3}},"canonical_sha256":"40015e59788ab1497d08085e39a7dd5b699add36cf60d477131f7714b2111ec9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"40015e59788ab1497d08085e39a7dd5b699add36cf60d477131f7714b2111ec9","first_computed_at":"2026-07-05T07:33:48.565676Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:33:48.565676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mlMobkmhbS1AWMqyM2GJrrEar0KTZyQZNR/EqE0l3IA1zLt43oL5KcGKUJpZHrZbsLAOh+0V766r1Y9jbUtWDA==","signature_status":"signed_v1","signed_at":"2026-07-05T07:33:48.566082Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.12996","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0569577920ce89c2a36b58dc5fc4cd5405cc70458686babf357ccede713ab281","sha256:7a12c72365ab1168673709e97308d7931b102cd907f498be1ab81fa7c6d39a73"],"state_sha256":"629302c4b8866e3482286eeb33d0eda88f6670b255115b51bfcb70164d9d3b68"}