{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:DYZ44SMWQZY46WJVRCMSNA24Y3","short_pith_number":"pith:DYZ44SMW","schema_version":"1.0","canonical_sha256":"1e33ce49968671cf5935889926835cc6df42dd1e4d4948e2496f2995430d1fa9","source":{"kind":"arxiv","id":"2407.02560","version":1},"attestation_state":"computed","paper":{"title":"When Could Abelian Fractional Topological Insulators Exist in Twisted MoTe$_2$ (and Other Systems)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Andrea Kouta Dagnino, B. Andrei Bernevig, Glenn Wagner, Jiabin Yu, Nicolas Regnault, Titus Neupert, Xiaodong Xu, Yi Jiang, Yves H. Kwan","submitted_at":"2024-07-02T18:00:01Z","abstract_excerpt":"Using comprehensive exact diagonalization calculations on $\\theta \\approx 3.7 ^{\\circ}$ twisted bilayer MoTe$_2$ ($t$MoTe$_2$), as well as idealized Landau level models also relevant for lower $\\theta$, we extract general principles for engineering fractional topological insulators (FTIs) in realistic situations. First, in a Landau level setup at $\\nu=1/3+1/3$, we investigate what features of the interaction destroy an FTI. For both pseudopotential interactions and realistic screened Coulomb interactions, we find that sufficient suppression of the short-range repulsion is needed for stabilizin"},"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":"2407.02560","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-07-02T18:00:01Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"9a9775ff0fd602fd176df586bb280ec0031232281d6d4ea8af764782a21bb6fe","abstract_canon_sha256":"2bf5fd5316afa0086d07041be893273c443df399c59e9bee96ad11a6bed68b5e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:39:38.513234Z","signature_b64":"KIbK7mq3R7aOaUEpbkaGsTu6o7Kz7Cv3kMcngcmH9ALpT60x0E30unPfFMzLsZwq20E1jKcrOGgmq/Z6ij9VBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e33ce49968671cf5935889926835cc6df42dd1e4d4948e2496f2995430d1fa9","last_reissued_at":"2026-07-05T08:39:38.512835Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:39:38.512835Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"When Could Abelian Fractional Topological Insulators Exist in Twisted MoTe$_2$ (and Other Systems)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Andrea Kouta Dagnino, B. Andrei Bernevig, Glenn Wagner, Jiabin Yu, Nicolas Regnault, Titus Neupert, Xiaodong Xu, Yi Jiang, Yves H. Kwan","submitted_at":"2024-07-02T18:00:01Z","abstract_excerpt":"Using comprehensive exact diagonalization calculations on $\\theta \\approx 3.7 ^{\\circ}$ twisted bilayer MoTe$_2$ ($t$MoTe$_2$), as well as idealized Landau level models also relevant for lower $\\theta$, we extract general principles for engineering fractional topological insulators (FTIs) in realistic situations. First, in a Landau level setup at $\\nu=1/3+1/3$, we investigate what features of the interaction destroy an FTI. For both pseudopotential interactions and realistic screened Coulomb interactions, we find that sufficient suppression of the short-range repulsion is needed for stabilizin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.02560","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/2407.02560/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":"2407.02560","created_at":"2026-07-05T08:39:38.512888+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.02560v1","created_at":"2026-07-05T08:39:38.512888+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.02560","created_at":"2026-07-05T08:39:38.512888+00:00"},{"alias_kind":"pith_short_12","alias_value":"DYZ44SMWQZY4","created_at":"2026-07-05T08:39:38.512888+00:00"},{"alias_kind":"pith_short_16","alias_value":"DYZ44SMWQZY46WJV","created_at":"2026-07-05T08:39:38.512888+00:00"},{"alias_kind":"pith_short_8","alias_value":"DYZ44SMW","created_at":"2026-07-05T08:39:38.512888+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.05410","citing_title":"Wilson-Loop-Ideal Bands and General Idealization","ref_index":105,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3","json":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3.json","graph_json":"https://pith.science/api/pith-number/DYZ44SMWQZY46WJVRCMSNA24Y3/graph.json","events_json":"https://pith.science/api/pith-number/DYZ44SMWQZY46WJVRCMSNA24Y3/events.json","paper":"https://pith.science/paper/DYZ44SMW"},"agent_actions":{"view_html":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3","download_json":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3.json","view_paper":"https://pith.science/paper/DYZ44SMW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.02560&json=true","fetch_graph":"https://pith.science/api/pith-number/DYZ44SMWQZY46WJVRCMSNA24Y3/graph.json","fetch_events":"https://pith.science/api/pith-number/DYZ44SMWQZY46WJVRCMSNA24Y3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3/action/storage_attestation","attest_author":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3/action/author_attestation","sign_citation":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3/action/citation_signature","submit_replication":"https://pith.science/pith/DYZ44SMWQZY46WJVRCMSNA24Y3/action/replication_record"}},"created_at":"2026-07-05T08:39:38.512888+00:00","updated_at":"2026-07-05T08:39:38.512888+00:00"}