{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GQNVFBFRAQZSNIMVABPVWSLJHV","short_pith_number":"pith:GQNVFBFR","schema_version":"1.0","canonical_sha256":"341b5284b1043326a195005f5b49693d59816da316d21828cbf69d8906fe3855","source":{"kind":"arxiv","id":"2511.10140","version":1},"attestation_state":"computed","paper":{"title":"Emergent electronic insulating states in a one-dimensional moir\\'e superlattice","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Dongjun Kang, Huizhen Wu, Jianfeng Bi, Kenji Watanabe, Masaki Minamikawa, Mikito Koshino, Naoto Nakatsuji, Ruige Dong, Ryosuke Okumura, SeokJae Yoo, Shaoqi Sun, Sihan Zhao, Takashi Taniguchi, Zihan Weng","submitted_at":"2025-11-13T09:52:05Z","abstract_excerpt":"Two-dimensional (2D) van der Waals (vdW) moir\\'e superlattices have provided a powerful knob to engineer a plethora of new quantum states. However, extending such moir\\'e engineering to one-dimensional (1D) vdW systems has remained challenging. Here we report the moir\\'e-engineered electronic insulating states in a new 1D moir\\'e superlattice, by crystallographically aligning an armchair single-walled carbon nanotube (SWNT) to 2D hexagonal boron nitride (hBN) substrate. Remarkably, we observe the emergence of pronounced insulating states at charge neutrality point (CNP), full and half moir\\'e "},"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":"2511.10140","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-11-13T09:52:05Z","cross_cats_sorted":[],"title_canon_sha256":"9255de66cd503a0da20168d50479d7e078943f698bb3f3365528f92ee1d007b6","abstract_canon_sha256":"0ab254ef130e5d8aec5ae8804f78ea909dd5a197a6d1c7b7b8175c07b548d147"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-10T01:09:20.279448Z","signature_b64":"eo2VBKM5lH+v8oWY38LQrVY1rTWneJJFWIHAOK4vTA+PTT+thYd4NChMiI4s6h9J0h27guG3NWZDZzlFhZs5BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"341b5284b1043326a195005f5b49693d59816da316d21828cbf69d8906fe3855","last_reissued_at":"2026-08-10T01:09:20.276937Z","signature_status":"signed_v1","first_computed_at":"2026-08-10T01:09:20.276937Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent electronic insulating states in a one-dimensional moir\\'e superlattice","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Dongjun Kang, Huizhen Wu, Jianfeng Bi, Kenji Watanabe, Masaki Minamikawa, Mikito Koshino, Naoto Nakatsuji, Ruige Dong, Ryosuke Okumura, SeokJae Yoo, Shaoqi Sun, Sihan Zhao, Takashi Taniguchi, Zihan Weng","submitted_at":"2025-11-13T09:52:05Z","abstract_excerpt":"Two-dimensional (2D) van der Waals (vdW) moir\\'e superlattices have provided a powerful knob to engineer a plethora of new quantum states. However, extending such moir\\'e engineering to one-dimensional (1D) vdW systems has remained challenging. Here we report the moir\\'e-engineered electronic insulating states in a new 1D moir\\'e superlattice, by crystallographically aligning an armchair single-walled carbon nanotube (SWNT) to 2D hexagonal boron nitride (hBN) substrate. Remarkably, we observe the emergence of pronounced insulating states at charge neutrality point (CNP), full and half moir\\'e "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.10140","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/2511.10140/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":"2511.10140","created_at":"2026-08-10T01:09:20.277895+00:00"},{"alias_kind":"arxiv_version","alias_value":"2511.10140v1","created_at":"2026-08-10T01:09:20.277895+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.10140","created_at":"2026-08-10T01:09:20.277895+00:00"},{"alias_kind":"pith_short_12","alias_value":"GQNVFBFRAQZS","created_at":"2026-08-10T01:09:20.277895+00:00"},{"alias_kind":"pith_short_16","alias_value":"GQNVFBFRAQZSNIMV","created_at":"2026-08-10T01:09:20.277895+00:00"},{"alias_kind":"pith_short_8","alias_value":"GQNVFBFR","created_at":"2026-08-10T01:09:20.277895+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.13532","citing_title":"Emergent topological phase from a one-dimensional network of defects","ref_index":73,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV","json":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV.json","graph_json":"https://pith.science/api/pith-number/GQNVFBFRAQZSNIMVABPVWSLJHV/graph.json","events_json":"https://pith.science/api/pith-number/GQNVFBFRAQZSNIMVABPVWSLJHV/events.json","paper":"https://pith.science/paper/GQNVFBFR"},"agent_actions":{"view_html":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV","download_json":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV.json","view_paper":"https://pith.science/paper/GQNVFBFR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2511.10140&json=true","fetch_graph":"https://pith.science/api/pith-number/GQNVFBFRAQZSNIMVABPVWSLJHV/graph.json","fetch_events":"https://pith.science/api/pith-number/GQNVFBFRAQZSNIMVABPVWSLJHV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV/action/storage_attestation","attest_author":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV/action/author_attestation","sign_citation":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV/action/citation_signature","submit_replication":"https://pith.science/pith/GQNVFBFRAQZSNIMVABPVWSLJHV/action/replication_record"}},"created_at":"2026-08-10T01:09:20.277895+00:00","updated_at":"2026-08-10T01:09:20.277895+00:00"}