{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:NWVXDYE4NG4RAWKTFVQFMCG5ZF","short_pith_number":"pith:NWVXDYE4","schema_version":"1.0","canonical_sha256":"6dab71e09c69b91059532d605608ddc958ac8198516906c58bd4a4f51268a3e1","source":{"kind":"arxiv","id":"cond-mat/9402108","version":1},"attestation_state":"computed","paper":{"title":"Randomness at the Edge: Theory of Quantum Hall transport at filling $\\nu=2/3$","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"C.L. Kane, J. Polchinski, M.P.A. Fisher","submitted_at":"1994-02-25T19:58:12Z","abstract_excerpt":"Current Luttinger liquid edge state theories for filling $\\nu=2/3$ predict a non-universal Hall conductance, in disagreement with experiment. Upon inclusion of random edge tunnelling we find a phase transition into a new disordered-dominated edge phase. An exact solution of the random model in this phase gives a quantized Hall conductance of 2/3 and a neutral mode propagating upstream. The presence of the neutral mode changes the predicted temperature dependence for tunnelling through a point contact from $T^{2/\\nu -2}$ to $T^2$."},"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":"cond-mat/9402108","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1994-02-25T19:58:12Z","cross_cats_sorted":[],"title_canon_sha256":"0bcb369b3004029c704d700789b41b21299358c02b30fc054422e6023ea82f68","abstract_canon_sha256":"fc760b61814a256697234539d150833b2fda8e1ee3a5ec3ffca11f99ba7e3598"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:56:37.912805Z","signature_b64":"OnuJxhCGDUAsvmWKFRJPJ+1avelqgzQnoD7niHFiS1banVc0VNRD2HpR7ecIPLKiLqKsFlmxwNyrkV6R2w5KBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6dab71e09c69b91059532d605608ddc958ac8198516906c58bd4a4f51268a3e1","last_reissued_at":"2026-07-04T15:56:37.912399Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:56:37.912399Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Randomness at the Edge: Theory of Quantum Hall transport at filling $\\nu=2/3$","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"C.L. Kane, J. Polchinski, M.P.A. Fisher","submitted_at":"1994-02-25T19:58:12Z","abstract_excerpt":"Current Luttinger liquid edge state theories for filling $\\nu=2/3$ predict a non-universal Hall conductance, in disagreement with experiment. Upon inclusion of random edge tunnelling we find a phase transition into a new disordered-dominated edge phase. An exact solution of the random model in this phase gives a quantized Hall conductance of 2/3 and a neutral mode propagating upstream. The presence of the neutral mode changes the predicted temperature dependence for tunnelling through a point contact from $T^{2/\\nu -2}$ to $T^2$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9402108","kind":"arxiv","version":1},"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/cond-mat/9402108/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":"cond-mat/9402108","created_at":"2026-07-04T15:56:37.912474+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9402108v1","created_at":"2026-07-04T15:56:37.912474+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9402108","created_at":"2026-07-04T15:56:37.912474+00:00"},{"alias_kind":"pith_short_12","alias_value":"NWVXDYE4NG4R","created_at":"2026-07-04T15:56:37.912474+00:00"},{"alias_kind":"pith_short_16","alias_value":"NWVXDYE4NG4RAWKT","created_at":"2026-07-04T15:56:37.912474+00:00"},{"alias_kind":"pith_short_8","alias_value":"NWVXDYE4","created_at":"2026-07-04T15:56:37.912474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.02128","citing_title":"Anyon delocalization transitions out of a disordered FQAH insulator","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF","json":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF.json","graph_json":"https://pith.science/api/pith-number/NWVXDYE4NG4RAWKTFVQFMCG5ZF/graph.json","events_json":"https://pith.science/api/pith-number/NWVXDYE4NG4RAWKTFVQFMCG5ZF/events.json","paper":"https://pith.science/paper/NWVXDYE4"},"agent_actions":{"view_html":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF","download_json":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF.json","view_paper":"https://pith.science/paper/NWVXDYE4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9402108&json=true","fetch_graph":"https://pith.science/api/pith-number/NWVXDYE4NG4RAWKTFVQFMCG5ZF/graph.json","fetch_events":"https://pith.science/api/pith-number/NWVXDYE4NG4RAWKTFVQFMCG5ZF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF/action/storage_attestation","attest_author":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF/action/author_attestation","sign_citation":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF/action/citation_signature","submit_replication":"https://pith.science/pith/NWVXDYE4NG4RAWKTFVQFMCG5ZF/action/replication_record"}},"created_at":"2026-07-04T15:56:37.912474+00:00","updated_at":"2026-07-04T15:56:37.912474+00:00"}