{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:VT7MCMMX45WUIYH4X3W54VNXHG","short_pith_number":"pith:VT7MCMMX","schema_version":"1.0","canonical_sha256":"acfec13197e76d4460fcbeedde55b739937fcca9d3d6c196e4a0cc3616d20975","source":{"kind":"arxiv","id":"1007.2030","version":3},"attestation_state":"computed","paper":{"title":"Anyon Condensation and Continuous Topological Phase Transitions in Non-Abelian Fractional Quantum Hall States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Maissam Barkeshli, Xiao-Gang Wen","submitted_at":"2010-07-13T04:08:14Z","abstract_excerpt":"We find a series of possible continuous quantum phase transitions between fractional quantum Hall (FQH) states at the same filling fraction in two-component quantum Hall systems. These can be driven by tuning the interlayer tunneling and/or interlayer repulsion. One side of the transition is the Halperin (p,p,p-3) Abelian two-component state while the other side is the non-Abelian Z4 parafermion (Read-Rezayi) state. We predict that the transition is a continuous transition in the 3D Ising class. The critical point is described by a Z2 gauged Ginzburg-Landau theory. These results have implicati"},"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":"1007.2030","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-13T04:08:14Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"eb4873e015a5a753c009d2bed19c47d6ebfa1d7cb374327274fc41663702928b","abstract_canon_sha256":"9e0d1908b340a7e83d3bd35d720ebddc6d113633ff9ce650b2dce55fbfba4537"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:06:22.700590Z","signature_b64":"zBs+kI3lpd30LQolQk4EGoDx+yG61biueyqeEOgpWOt3+40dp7WcYG+P/H/n0UVtfa54CX2pPzfj+gQ8PthZCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"acfec13197e76d4460fcbeedde55b739937fcca9d3d6c196e4a0cc3616d20975","last_reissued_at":"2026-05-18T02:06:22.699832Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:06:22.699832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anyon Condensation and Continuous Topological Phase Transitions in Non-Abelian Fractional Quantum Hall States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Maissam Barkeshli, Xiao-Gang Wen","submitted_at":"2010-07-13T04:08:14Z","abstract_excerpt":"We find a series of possible continuous quantum phase transitions between fractional quantum Hall (FQH) states at the same filling fraction in two-component quantum Hall systems. These can be driven by tuning the interlayer tunneling and/or interlayer repulsion. One side of the transition is the Halperin (p,p,p-3) Abelian two-component state while the other side is the non-Abelian Z4 parafermion (Read-Rezayi) state. We predict that the transition is a continuous transition in the 3D Ising class. The critical point is described by a Z2 gauged Ginzburg-Landau theory. These results have implicati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.2030","kind":"arxiv","version":3},"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":"1007.2030","created_at":"2026-05-18T02:06:22.699935+00:00"},{"alias_kind":"arxiv_version","alias_value":"1007.2030v3","created_at":"2026-05-18T02:06:22.699935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.2030","created_at":"2026-05-18T02:06:22.699935+00:00"},{"alias_kind":"pith_short_12","alias_value":"VT7MCMMX45WU","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"VT7MCMMX45WUIYH4","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"VT7MCMMX","created_at":"2026-05-18T12:26:15.391820+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/VT7MCMMX45WUIYH4X3W54VNXHG","json":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG.json","graph_json":"https://pith.science/api/pith-number/VT7MCMMX45WUIYH4X3W54VNXHG/graph.json","events_json":"https://pith.science/api/pith-number/VT7MCMMX45WUIYH4X3W54VNXHG/events.json","paper":"https://pith.science/paper/VT7MCMMX"},"agent_actions":{"view_html":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG","download_json":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG.json","view_paper":"https://pith.science/paper/VT7MCMMX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1007.2030&json=true","fetch_graph":"https://pith.science/api/pith-number/VT7MCMMX45WUIYH4X3W54VNXHG/graph.json","fetch_events":"https://pith.science/api/pith-number/VT7MCMMX45WUIYH4X3W54VNXHG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG/action/storage_attestation","attest_author":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG/action/author_attestation","sign_citation":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG/action/citation_signature","submit_replication":"https://pith.science/pith/VT7MCMMX45WUIYH4X3W54VNXHG/action/replication_record"}},"created_at":"2026-05-18T02:06:22.699935+00:00","updated_at":"2026-05-18T02:06:22.699935+00:00"}