{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:QV5VDGTMSMSJPUVS3MWGE2N44N","short_pith_number":"pith:QV5VDGTM","schema_version":"1.0","canonical_sha256":"857b519a6c932497d2b2db2c6269bce3613a8b5d92d34a4f65b77d29c28fb56f","source":{"kind":"arxiv","id":"2405.08386","version":5},"attestation_state":"computed","paper":{"title":"Robust non-Abelian even-denominator fractional Chern insulator in twisted bilayer MoTe$_2$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. N. Sheng, Feng Chen, Wei-Wei Luo, Wei Zhu","submitted_at":"2024-05-14T07:34:07Z","abstract_excerpt":"A recent experiment observes a series of quantum spin Hall effects in transition metal dichalcogenide moir\\'e MoTe$_2$ [K. Kang, et. al, Nature 628, 522-526 (2024)]. Among them, the vanishing Hall signal at the filling factor $\\nu=3$ implies a possible realization of a time-reversal pair of the even-denominator fractional Chern insulators (FCIs). Inspired by this discovery, we investigate whether a robust incompressible quantum Hall liquid can be stabilized in the half-filled Chern band of twisted MoTe$_2$ bilayers. We use the continuum model with parameters relevant to twisted MoTe$_2$ bilaye"},"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":"2405.08386","kind":"arxiv","version":5},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-05-14T07:34:07Z","cross_cats_sorted":[],"title_canon_sha256":"ab5c344d6a52cd0b301a3bba567b06f88ca0a57b8a7f997fbf95de8d941a08b1","abstract_canon_sha256":"c259f8053fb5ee6460c0d621e85dfa9bea1676c873cc8b66215781d6e651939c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:16:58.304312Z","signature_b64":"rlWex3UfuhyhkG7MqLgcIaoIqAsO5vHM2JLfzctj14ZvYG6jmX8tDLJlm2sUymxaVOADgxmBMvCoy4AWi3sgAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"857b519a6c932497d2b2db2c6269bce3613a8b5d92d34a4f65b77d29c28fb56f","last_reissued_at":"2026-07-05T10:16:58.303809Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:16:58.303809Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Robust non-Abelian even-denominator fractional Chern insulator in twisted bilayer MoTe$_2$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. N. Sheng, Feng Chen, Wei-Wei Luo, Wei Zhu","submitted_at":"2024-05-14T07:34:07Z","abstract_excerpt":"A recent experiment observes a series of quantum spin Hall effects in transition metal dichalcogenide moir\\'e MoTe$_2$ [K. Kang, et. al, Nature 628, 522-526 (2024)]. Among them, the vanishing Hall signal at the filling factor $\\nu=3$ implies a possible realization of a time-reversal pair of the even-denominator fractional Chern insulators (FCIs). Inspired by this discovery, we investigate whether a robust incompressible quantum Hall liquid can be stabilized in the half-filled Chern band of twisted MoTe$_2$ bilayers. We use the continuum model with parameters relevant to twisted MoTe$_2$ bilaye"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.08386","kind":"arxiv","version":5},"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/2405.08386/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":"2405.08386","created_at":"2026-07-05T10:16:58.303870+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.08386v5","created_at":"2026-07-05T10:16:58.303870+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.08386","created_at":"2026-07-05T10:16:58.303870+00:00"},{"alias_kind":"pith_short_12","alias_value":"QV5VDGTMSMSJ","created_at":"2026-07-05T10:16:58.303870+00:00"},{"alias_kind":"pith_short_16","alias_value":"QV5VDGTMSMSJPUVS","created_at":"2026-07-05T10:16:58.303870+00:00"},{"alias_kind":"pith_short_8","alias_value":"QV5VDGTM","created_at":"2026-07-05T10:16:58.303870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.02128","citing_title":"Quantum phase diagram and non-abelian Moore-Read state in double twisted bilayer graphene","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N","json":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N.json","graph_json":"https://pith.science/api/pith-number/QV5VDGTMSMSJPUVS3MWGE2N44N/graph.json","events_json":"https://pith.science/api/pith-number/QV5VDGTMSMSJPUVS3MWGE2N44N/events.json","paper":"https://pith.science/paper/QV5VDGTM"},"agent_actions":{"view_html":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N","download_json":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N.json","view_paper":"https://pith.science/paper/QV5VDGTM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.08386&json=true","fetch_graph":"https://pith.science/api/pith-number/QV5VDGTMSMSJPUVS3MWGE2N44N/graph.json","fetch_events":"https://pith.science/api/pith-number/QV5VDGTMSMSJPUVS3MWGE2N44N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N/action/storage_attestation","attest_author":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N/action/author_attestation","sign_citation":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N/action/citation_signature","submit_replication":"https://pith.science/pith/QV5VDGTMSMSJPUVS3MWGE2N44N/action/replication_record"}},"created_at":"2026-07-05T10:16:58.303870+00:00","updated_at":"2026-07-05T10:16:58.303870+00:00"}