{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:VA32XJ3FBKOY2ZJKLDV5KTWE7A","short_pith_number":"pith:VA32XJ3F","schema_version":"1.0","canonical_sha256":"a837aba7650a9d8d652a58ebd54ec4f82a96496306b436e82ce5303bbcf633b8","source":{"kind":"arxiv","id":"1906.00983","version":2},"attestation_state":"computed","paper":{"title":"Landau-Ginzburg Theories of Non-Abelian Quantum Hall States from Non-Abelian Bosonization","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":"Eduardo Fradkin, Hart Goldman, Ramanjit Sohal","submitted_at":"2019-06-03T18:00:07Z","abstract_excerpt":"It is an important open problem to understand the landscape of non-Abelian fractional quantum Hall phases which can be obtained starting from physically motivated theories of Abelian composite particles. We show that progress on this problem can be made using recently proposed non-Abelian bosonization dualities in 2+1 dimensions, which morally relate $U(N)_k$ and $SU(k)_{-N}$ Chern-Simons-matter theories. The advantage of these dualities is that regions of the phase diagram which may be obscure on one side of the duality can be accessed by condensing local operators on the other side. Starting"},"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":"1906.00983","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2019-06-03T18:00:07Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"b707d31e2ea2b13d75d1a350c6b2ba9181a457c14a8043566723ad94824640fc","abstract_canon_sha256":"c1d4bbc9db91a51194ccfddab914464d5d7744adc18f8e6617e4b43797fd4fde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:03:47.498157Z","signature_b64":"kAVZUQTaRISnxuG/rqXi3xzlH0tCoS9qlpxsKOkrjFFgvTA5PAgywES3epi9lyjf8Zb5sN77W7s/rYDo11CDBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a837aba7650a9d8d652a58ebd54ec4f82a96496306b436e82ce5303bbcf633b8","last_reissued_at":"2026-07-05T00:03:47.497672Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:03:47.497672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Landau-Ginzburg Theories of Non-Abelian Quantum Hall States from Non-Abelian Bosonization","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":"Eduardo Fradkin, Hart Goldman, Ramanjit Sohal","submitted_at":"2019-06-03T18:00:07Z","abstract_excerpt":"It is an important open problem to understand the landscape of non-Abelian fractional quantum Hall phases which can be obtained starting from physically motivated theories of Abelian composite particles. We show that progress on this problem can be made using recently proposed non-Abelian bosonization dualities in 2+1 dimensions, which morally relate $U(N)_k$ and $SU(k)_{-N}$ Chern-Simons-matter theories. The advantage of these dualities is that regions of the phase diagram which may be obscure on one side of the duality can be accessed by condensing local operators on the other side. Starting"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.00983","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1906.00983/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1906.00983","created_at":"2026-07-05T00:03:47.497732+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.00983v2","created_at":"2026-07-05T00:03:47.497732+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.00983","created_at":"2026-07-05T00:03:47.497732+00:00"},{"alias_kind":"pith_short_12","alias_value":"VA32XJ3FBKOY","created_at":"2026-07-05T00:03:47.497732+00:00"},{"alias_kind":"pith_short_16","alias_value":"VA32XJ3FBKOY2ZJK","created_at":"2026-07-05T00:03:47.497732+00:00"},{"alias_kind":"pith_short_8","alias_value":"VA32XJ3F","created_at":"2026-07-05T00:03:47.497732+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2506.23155","citing_title":"Homomorphism, substructure, and ideal: Elementary but rigorous aspects of renormalization group or hierarchical structure of topological orders","ref_index":158,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A","json":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A.json","graph_json":"https://pith.science/api/pith-number/VA32XJ3FBKOY2ZJKLDV5KTWE7A/graph.json","events_json":"https://pith.science/api/pith-number/VA32XJ3FBKOY2ZJKLDV5KTWE7A/events.json","paper":"https://pith.science/paper/VA32XJ3F"},"agent_actions":{"view_html":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A","download_json":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A.json","view_paper":"https://pith.science/paper/VA32XJ3F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.00983&json=true","fetch_graph":"https://pith.science/api/pith-number/VA32XJ3FBKOY2ZJKLDV5KTWE7A/graph.json","fetch_events":"https://pith.science/api/pith-number/VA32XJ3FBKOY2ZJKLDV5KTWE7A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A/action/storage_attestation","attest_author":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A/action/author_attestation","sign_citation":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A/action/citation_signature","submit_replication":"https://pith.science/pith/VA32XJ3FBKOY2ZJKLDV5KTWE7A/action/replication_record"}},"created_at":"2026-07-05T00:03:47.497732+00:00","updated_at":"2026-07-05T00:03:47.497732+00:00"}