{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:2IVWR6WFGZ67WZSHRZHNOYA36F","short_pith_number":"pith:2IVWR6WF","schema_version":"1.0","canonical_sha256":"d22b68fac5367dfb66478e4ed7601bf162a7a16fbfc845c09c1c691bde966516","source":{"kind":"arxiv","id":"1109.2095","version":3},"attestation_state":"computed","paper":{"title":"Edge Mode Combinations in the Entanglement Spectra of Non-Abelian Fractional Quantum Hall States on the Torus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Andreas M. Laeuchli, Emil J. Bergholtz, Heng Fan, Zhao Liu","submitted_at":"2011-09-09T19:05:44Z","abstract_excerpt":"We present a detailed analysis of bi-partite entanglement in the non-Abelian Moore-Read fractional quantum Hall state of bosons and fermions on the torus. In particular, we show that the entanglement spectra can be decomposed into intricate combinations of different sectors of the conformal field theory describing the edge physics, and that the edge level counting and tower structure can be microscopically understood by considering the vicinity of the thin-torus limit. We also find that the boundary entropy density of the Moore-Read state is markedly higher than in the Laughlin states investig"},"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":"1109.2095","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-09-09T19:05:44Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"9953a01a5db1ad2a4f5dd9ff076427fe29f1139ecde4058d39a3b60bda33976a","abstract_canon_sha256":"eafc58d756d8b4241bc827414029b7f3831459d585f8e81de00f0be9f8f8c19a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:16.804769Z","signature_b64":"141U1jr2SyvY4jM2pkQ5S0G4v1o49wlhUHW40pNdX5jYo7hvEMqC1+qJzDqizWQBKnsZuHoiCJGbqEZ9zYw3Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d22b68fac5367dfb66478e4ed7601bf162a7a16fbfc845c09c1c691bde966516","last_reissued_at":"2026-05-18T04:04:16.803984Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:16.803984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Edge Mode Combinations in the Entanglement Spectra of Non-Abelian Fractional Quantum Hall States on the Torus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Andreas M. Laeuchli, Emil J. Bergholtz, Heng Fan, Zhao Liu","submitted_at":"2011-09-09T19:05:44Z","abstract_excerpt":"We present a detailed analysis of bi-partite entanglement in the non-Abelian Moore-Read fractional quantum Hall state of bosons and fermions on the torus. In particular, we show that the entanglement spectra can be decomposed into intricate combinations of different sectors of the conformal field theory describing the edge physics, and that the edge level counting and tower structure can be microscopically understood by considering the vicinity of the thin-torus limit. We also find that the boundary entropy density of the Moore-Read state is markedly higher than in the Laughlin states investig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.2095","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":"1109.2095","created_at":"2026-05-18T04:04:16.804104+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.2095v3","created_at":"2026-05-18T04:04:16.804104+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.2095","created_at":"2026-05-18T04:04:16.804104+00:00"},{"alias_kind":"pith_short_12","alias_value":"2IVWR6WFGZ67","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"2IVWR6WFGZ67WZSH","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"2IVWR6WF","created_at":"2026-05-18T12:26:18.847500+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/2IVWR6WFGZ67WZSHRZHNOYA36F","json":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F.json","graph_json":"https://pith.science/api/pith-number/2IVWR6WFGZ67WZSHRZHNOYA36F/graph.json","events_json":"https://pith.science/api/pith-number/2IVWR6WFGZ67WZSHRZHNOYA36F/events.json","paper":"https://pith.science/paper/2IVWR6WF"},"agent_actions":{"view_html":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F","download_json":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F.json","view_paper":"https://pith.science/paper/2IVWR6WF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.2095&json=true","fetch_graph":"https://pith.science/api/pith-number/2IVWR6WFGZ67WZSHRZHNOYA36F/graph.json","fetch_events":"https://pith.science/api/pith-number/2IVWR6WFGZ67WZSHRZHNOYA36F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F/action/storage_attestation","attest_author":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F/action/author_attestation","sign_citation":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F/action/citation_signature","submit_replication":"https://pith.science/pith/2IVWR6WFGZ67WZSHRZHNOYA36F/action/replication_record"}},"created_at":"2026-05-18T04:04:16.804104+00:00","updated_at":"2026-05-18T04:04:16.804104+00:00"}