{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:QBN5MXGUUO5E3CAEIDTHGJ2B4L","short_pith_number":"pith:QBN5MXGU","schema_version":"1.0","canonical_sha256":"805bd65cd4a3ba4d880440e6732741e2d6e698279e06d39c463943754364abbd","source":{"kind":"arxiv","id":"2311.05568","version":2},"attestation_state":"computed","paper":{"title":"Anomalous Hall Crystals in Rhombohedral Multilayer Graphene I: Interaction-Driven Chern Bands and Fractional Quantum Hall States at Zero Magnetic Field","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Ashvin Vishwanath, Daniel E. Parker, Junkai Dong, Michael P. Zaletel, Taige Wang, Tianle Wang, Tomohiro Soejima","submitted_at":"2023-11-09T18:23:41Z","abstract_excerpt":"Recent experiments on rhombohedral pentalayer graphene flakes with a substrate induced moir\\'e potential have identified both Chern insulators and fractional Quantum Hall states in the absence of an applied magnetic field. Surprisingly, these states are observed in strong displacement fields where the effects of the moir\\'e lattice are weak, and seem to be readily accessed without fine-tuning. To address these experimental puzzles we study an interacting model of electrons in this geometry, first within the self-consistent Hartree-Fock (SCHF) approximation. We find an isolated Chern band with "},"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":"2311.05568","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-09T18:23:41Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"6f6bfc3d134702a356a313ca77a5b45f81135a324fd7c3c15e7192f02e052671","abstract_canon_sha256":"6773545d6436dc40ee103266daca051d00043052276a97d4edba8865f5e739bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:35:06.980236Z","signature_b64":"wJ7x5qt2pQZ49UFyllnJQ3ps82qtPA2stFEQra/nmCAqsBp7GDmmoLqYLj0TikDJJwDWDiecNDSEjqutpZDIAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"805bd65cd4a3ba4d880440e6732741e2d6e698279e06d39c463943754364abbd","last_reissued_at":"2026-07-05T09:35:06.979760Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:35:06.979760Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous Hall Crystals in Rhombohedral Multilayer Graphene I: Interaction-Driven Chern Bands and Fractional Quantum Hall States at Zero Magnetic Field","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Ashvin Vishwanath, Daniel E. Parker, Junkai Dong, Michael P. Zaletel, Taige Wang, Tianle Wang, Tomohiro Soejima","submitted_at":"2023-11-09T18:23:41Z","abstract_excerpt":"Recent experiments on rhombohedral pentalayer graphene flakes with a substrate induced moir\\'e potential have identified both Chern insulators and fractional Quantum Hall states in the absence of an applied magnetic field. Surprisingly, these states are observed in strong displacement fields where the effects of the moir\\'e lattice are weak, and seem to be readily accessed without fine-tuning. To address these experimental puzzles we study an interacting model of electrons in this geometry, first within the self-consistent Hartree-Fock (SCHF) approximation. We find an isolated Chern band with "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.05568","kind":"arxiv","version":2},"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/2311.05568/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":"2311.05568","created_at":"2026-07-05T09:35:06.979813+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.05568v2","created_at":"2026-07-05T09:35:06.979813+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.05568","created_at":"2026-07-05T09:35:06.979813+00:00"},{"alias_kind":"pith_short_12","alias_value":"QBN5MXGUUO5E","created_at":"2026-07-05T09:35:06.979813+00:00"},{"alias_kind":"pith_short_16","alias_value":"QBN5MXGUUO5E3CAE","created_at":"2026-07-05T09:35:06.979813+00:00"},{"alias_kind":"pith_short_8","alias_value":"QBN5MXGU","created_at":"2026-07-05T09:35:06.979813+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2407.12198","citing_title":"Doping-induced Quantum Anomalous Hall Crystals and Topological Domain Walls","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2410.05384","citing_title":"Chiral superconductivity from parent Chern band and its non-Abelian generalization","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2504.11177","citing_title":"Pressure-Tunable Generalized Wigner Crystal and Fractional Chern Insulator in twisted MoTe$_2$","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L","json":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L.json","graph_json":"https://pith.science/api/pith-number/QBN5MXGUUO5E3CAEIDTHGJ2B4L/graph.json","events_json":"https://pith.science/api/pith-number/QBN5MXGUUO5E3CAEIDTHGJ2B4L/events.json","paper":"https://pith.science/paper/QBN5MXGU"},"agent_actions":{"view_html":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L","download_json":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L.json","view_paper":"https://pith.science/paper/QBN5MXGU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.05568&json=true","fetch_graph":"https://pith.science/api/pith-number/QBN5MXGUUO5E3CAEIDTHGJ2B4L/graph.json","fetch_events":"https://pith.science/api/pith-number/QBN5MXGUUO5E3CAEIDTHGJ2B4L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L/action/storage_attestation","attest_author":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L/action/author_attestation","sign_citation":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L/action/citation_signature","submit_replication":"https://pith.science/pith/QBN5MXGUUO5E3CAEIDTHGJ2B4L/action/replication_record"}},"created_at":"2026-07-05T09:35:06.979813+00:00","updated_at":"2026-07-05T09:35:06.979813+00:00"}