{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:5WRDIHIELCX3HKTVTQPFHBFEVW","short_pith_number":"pith:5WRDIHIE","schema_version":"1.0","canonical_sha256":"eda2341d0458afb3aa759c1e5384a4ada340b022632dddc62b24ffd83b7b8413","source":{"kind":"arxiv","id":"1902.04173","version":2},"attestation_state":"computed","paper":{"title":"Parton construction of particle-hole-conjugate Read-Rezayi parafermion fractional quantum Hall states and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Ajit C. Balram, Maissam Barkeshli, Mark S. Rudner","submitted_at":"2019-02-11T22:31:18Z","abstract_excerpt":"The Read-Rezayi (RR) parafermion states form a series of exotic non-Abelian fractional quantum Hall (FQH) states at filling $\\nu = k/(k+2)$. Computationally, the wave functions of these states are prohibitively expensive to generate for large systems. We introduce a series of parton states, denoted \"$\\bar{2}^{k}1^{k+1}$,\" and show that they lie in the same universality classes as the particle-hole-conjugate RR (\"anti-RR\") states. Our analytical results imply that a $(U(1)_{k+1} \\times U(2k)_{-1})/(SU(k)_{-2} \\times U(1)_{-1})$ coset conformal field theory describes the edge excitations of the "},"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":"1902.04173","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2019-02-11T22:31:18Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"2f82aecab23dac041dc57be5771be022c07ec4033b794bf9801a78c894ebe221","abstract_canon_sha256":"3612e473de72e2b1a174ad01e0e5bb879f3863c34f6a1ea656c9a647f595728b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:23.885574Z","signature_b64":"jU5oq+ryOkMWQSyto2Fyw81W8NK9lcGp1xMnNeCwtiGJ1HnzBkpEPAY8ZApPLOaPuDP/OPF/9ypJ/NobIQXvAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eda2341d0458afb3aa759c1e5384a4ada340b022632dddc62b24ffd83b7b8413","last_reissued_at":"2026-05-17T23:42:23.884897Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:23.884897Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Parton construction of particle-hole-conjugate Read-Rezayi parafermion fractional quantum Hall states and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Ajit C. Balram, Maissam Barkeshli, Mark S. Rudner","submitted_at":"2019-02-11T22:31:18Z","abstract_excerpt":"The Read-Rezayi (RR) parafermion states form a series of exotic non-Abelian fractional quantum Hall (FQH) states at filling $\\nu = k/(k+2)$. Computationally, the wave functions of these states are prohibitively expensive to generate for large systems. We introduce a series of parton states, denoted \"$\\bar{2}^{k}1^{k+1}$,\" and show that they lie in the same universality classes as the particle-hole-conjugate RR (\"anti-RR\") states. Our analytical results imply that a $(U(1)_{k+1} \\times U(2k)_{-1})/(SU(k)_{-2} \\times U(1)_{-1})$ coset conformal field theory describes the edge excitations of the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.04173","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":"1902.04173","created_at":"2026-05-17T23:42:23.885003+00:00"},{"alias_kind":"arxiv_version","alias_value":"1902.04173v2","created_at":"2026-05-17T23:42:23.885003+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.04173","created_at":"2026-05-17T23:42:23.885003+00:00"},{"alias_kind":"pith_short_12","alias_value":"5WRDIHIELCX3","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_16","alias_value":"5WRDIHIELCX3HKTV","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_8","alias_value":"5WRDIHIE","created_at":"2026-05-18T12:33:10.108867+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/5WRDIHIELCX3HKTVTQPFHBFEVW","json":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW.json","graph_json":"https://pith.science/api/pith-number/5WRDIHIELCX3HKTVTQPFHBFEVW/graph.json","events_json":"https://pith.science/api/pith-number/5WRDIHIELCX3HKTVTQPFHBFEVW/events.json","paper":"https://pith.science/paper/5WRDIHIE"},"agent_actions":{"view_html":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW","download_json":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW.json","view_paper":"https://pith.science/paper/5WRDIHIE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1902.04173&json=true","fetch_graph":"https://pith.science/api/pith-number/5WRDIHIELCX3HKTVTQPFHBFEVW/graph.json","fetch_events":"https://pith.science/api/pith-number/5WRDIHIELCX3HKTVTQPFHBFEVW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW/action/storage_attestation","attest_author":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW/action/author_attestation","sign_citation":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW/action/citation_signature","submit_replication":"https://pith.science/pith/5WRDIHIELCX3HKTVTQPFHBFEVW/action/replication_record"}},"created_at":"2026-05-17T23:42:23.885003+00:00","updated_at":"2026-05-17T23:42:23.885003+00:00"}