{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:67FRY4I5TODTHFIREVV2DZU7WO","short_pith_number":"pith:67FRY4I5","schema_version":"1.0","canonical_sha256":"f7cb1c711d9b87339511256ba1e69fb39ca7fd4a83d8a0fab8c36429437236fd","source":{"kind":"arxiv","id":"1801.10149","version":2},"attestation_state":"computed","paper":{"title":"Theory of Disordered $\\nu = 5/2$ Quantum Thermal Hall State: Emergent Symmetry and Phase Diagram","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.mes-hall","authors_text":"Biao Lian, Juven Wang","submitted_at":"2018-01-30T18:59:38Z","abstract_excerpt":"Fractional quantum Hall (FQH) system at Landau level filling fraction $\\nu=5/2$ has long been suggested to be non-Abelian, either Pfaffian (Pf) or antiPfaffian (APf) states by numerical studies, both with quantized Hall conductance $\\sigma_{xy}=5e^2/2h$. Thermal Hall conductances of the Pf and APf states are quantized at $\\kappa_{xy}=7/2$ and $\\kappa_{xy}=3/2$ respectively in a proper unit. However, a recent experiment shows the thermal Hall conductance of $\\nu=5/2$ FQH state is $\\kappa_{xy}=5/2$. It has been speculated that the system contains random Pf and APf domains driven by disorders, an"},"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":"1801.10149","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-30T18:59:38Z","cross_cats_sorted":["cond-mat.str-el","hep-th"],"title_canon_sha256":"80fa92aa391aab6cdb10776f2b42b32adca0a6d84987c8b8e847649c8bfbb13f","abstract_canon_sha256":"43b47e69f82e1b82e2468a5ba84a6004c2639a51e0daf0f91377357b1f8657e7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:25.313011Z","signature_b64":"xb0Ol+B2TKg2bF8lIwnb7X5nGmiS7EM4sMbDKW5DVWFaVUoYmb1SRyLLyzGal5Ut7XAdNscUmB1zXaJOVuVfDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7cb1c711d9b87339511256ba1e69fb39ca7fd4a83d8a0fab8c36429437236fd","last_reissued_at":"2026-05-18T00:18:25.312398Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:25.312398Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of Disordered $\\nu = 5/2$ Quantum Thermal Hall State: Emergent Symmetry and Phase Diagram","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.mes-hall","authors_text":"Biao Lian, Juven Wang","submitted_at":"2018-01-30T18:59:38Z","abstract_excerpt":"Fractional quantum Hall (FQH) system at Landau level filling fraction $\\nu=5/2$ has long been suggested to be non-Abelian, either Pfaffian (Pf) or antiPfaffian (APf) states by numerical studies, both with quantized Hall conductance $\\sigma_{xy}=5e^2/2h$. Thermal Hall conductances of the Pf and APf states are quantized at $\\kappa_{xy}=7/2$ and $\\kappa_{xy}=3/2$ respectively in a proper unit. However, a recent experiment shows the thermal Hall conductance of $\\nu=5/2$ FQH state is $\\kappa_{xy}=5/2$. It has been speculated that the system contains random Pf and APf domains driven by disorders, an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.10149","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":""},"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":"1801.10149","created_at":"2026-05-18T00:18:25.312488+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.10149v2","created_at":"2026-05-18T00:18:25.312488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.10149","created_at":"2026-05-18T00:18:25.312488+00:00"},{"alias_kind":"pith_short_12","alias_value":"67FRY4I5TODT","created_at":"2026-05-18T12:32:08.215937+00:00"},{"alias_kind":"pith_short_16","alias_value":"67FRY4I5TODTHFIR","created_at":"2026-05-18T12:32:08.215937+00:00"},{"alias_kind":"pith_short_8","alias_value":"67FRY4I5","created_at":"2026-05-18T12:32:08.215937+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO","json":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO.json","graph_json":"https://pith.science/api/pith-number/67FRY4I5TODTHFIREVV2DZU7WO/graph.json","events_json":"https://pith.science/api/pith-number/67FRY4I5TODTHFIREVV2DZU7WO/events.json","paper":"https://pith.science/paper/67FRY4I5"},"agent_actions":{"view_html":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO","download_json":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO.json","view_paper":"https://pith.science/paper/67FRY4I5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.10149&json=true","fetch_graph":"https://pith.science/api/pith-number/67FRY4I5TODTHFIREVV2DZU7WO/graph.json","fetch_events":"https://pith.science/api/pith-number/67FRY4I5TODTHFIREVV2DZU7WO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO/action/storage_attestation","attest_author":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO/action/author_attestation","sign_citation":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO/action/citation_signature","submit_replication":"https://pith.science/pith/67FRY4I5TODTHFIREVV2DZU7WO/action/replication_record"}},"created_at":"2026-05-18T00:18:25.312488+00:00","updated_at":"2026-05-18T00:18:25.312488+00:00"}