{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:Z4HCTGDZSJFRPKZ43LLE7LJX6W","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":"7ba9dc64cdccf46c9c5c8e3a9b0b5d96fa9c0617d8125b4118cc1abc44257810","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":"2022-12-26T02:41:04Z","title_canon_sha256":"ec08e6d000a265670682de416f19ce61ff96fc4519b7990e5954188810a0ed83"},"schema_version":"1.0","source":{"id":"2212.12993","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.12993","created_at":"2026-07-05T06:42:58Z"},{"alias_kind":"arxiv_version","alias_value":"2212.12993v3","created_at":"2026-07-05T06:42:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.12993","created_at":"2026-07-05T06:42:58Z"},{"alias_kind":"pith_short_12","alias_value":"Z4HCTGDZSJFR","created_at":"2026-07-05T06:42:58Z"},{"alias_kind":"pith_short_16","alias_value":"Z4HCTGDZSJFRPKZ4","created_at":"2026-07-05T06:42:58Z"},{"alias_kind":"pith_short_8","alias_value":"Z4HCTGDZ","created_at":"2026-07-05T06:42:58Z"}],"graph_snapshots":[{"event_id":"sha256:1b19c6feddeedc55ada373b8b76663a326df751af3f773c2e92803e00b763304","target":"graph","created_at":"2026-07-05T06:42:58Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2212.12993/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In contemporary physics, especially in condensed matter physics, fermionic topological order and its protected edge modes are one of the most important objects. In this work, we propose a systematic construction of the cylinder partition corresponding to the fermionic fractional quantum Hall effect (FQHE) and a general mechanism for obtaining the candidates of the protected edge modes. In our construction, when the underlying conformal field theory has the $Z_{2}$ duality defects corresponding to the fermionic $Z_{2}$ electric particle, we show that the FQH partition function has a fermionic T","authors_text":"Bo Yang, 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":"2022-12-26T02:41:04Z","title":"Fermionic fractional quantum Hall states: A modern approach to systems with bulk-edge correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.12993","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":"sha256:79e076ef3bb3388b00c22610bdf8555649183f719ee97ac8cbdbfeb2a6c8e428","target":"record","created_at":"2026-07-05T06:42:58Z","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":"7ba9dc64cdccf46c9c5c8e3a9b0b5d96fa9c0617d8125b4118cc1abc44257810","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":"2022-12-26T02:41:04Z","title_canon_sha256":"ec08e6d000a265670682de416f19ce61ff96fc4519b7990e5954188810a0ed83"},"schema_version":"1.0","source":{"id":"2212.12993","kind":"arxiv","version":3}},"canonical_sha256":"cf0e299879924b17ab3cdad64fad37f5a4994061a611ff74c47f950a231f4a4e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cf0e299879924b17ab3cdad64fad37f5a4994061a611ff74c47f950a231f4a4e","first_computed_at":"2026-07-05T06:42:58.134980Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:42:58.134980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HvbJuGu4Oi+8av+J6uUalfOz2ngveW1LFOUqts6zscU/3a60qD+0knTFcXDXbKp7oMStzbrNjqRiiece9iSuAA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:42:58.135486Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.12993","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:79e076ef3bb3388b00c22610bdf8555649183f719ee97ac8cbdbfeb2a6c8e428","sha256:1b19c6feddeedc55ada373b8b76663a326df751af3f773c2e92803e00b763304"],"state_sha256":"0ccfa329c9dc3c32022cf72a6206f394d7d7cea07dbece6301d5e9f7a420862b"}