{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KQXBOHHT2YHQR2Z4KFFUA4YMMM","short_pith_number":"pith:KQXBOHHT","schema_version":"1.0","canonical_sha256":"542e171cf3d60f08eb3c514b40730c63160ca871aba064985b7a5bcba5ef503d","source":{"kind":"arxiv","id":"2406.08655","version":2},"attestation_state":"computed","paper":{"title":"Interacting holes in a gated WSe$_2$ quantum channel: valley correlations and zigzag Wigner crystal","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Adina Luican-Mayer, Daniel Miravet, Jaros{\\l}aw Paw{\\l}owski, Justin Boddison-Chouinard, Louis Gaudreau, Maciej Bieniek, Marek Korkusinski, Pawel Hawrylak","submitted_at":"2024-06-12T21:36:15Z","abstract_excerpt":"We present a theory of interacting valence holes in a gate-defined one-dimensional quantum channel in a single layer of a transition metal dichalcogenide material WSe$_2$. Based on a microscopic atomistic tight-binding model and Hartree-Fock and exact configuration-interaction tools we demonstrate the possibility of symmetry-broken valley polarized states for strongly interacting holes. The interplay between interactions, perpendicular magnetic field, and the lateral confinement asymmetry together with the strong Rashba spin-orbit coupling present in WSe$_2$ material is analyzed, and its impac"},"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":"2406.08655","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-06-12T21:36:15Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"8d6698511d3e375dabc240334a15ce4ef4d5900ba3a92025a12badd8a1308977","abstract_canon_sha256":"530fc3ca5536ce82879357f954f8b0009edf12c5344beef5269a36299de808d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:11:26.783020Z","signature_b64":"ArneIo49MXf1h9hOLs9DsUtw0b4gXrS5+7T2y2g1wL4K8Z6OzsnoAWKkemY+oVOuWEPJbwmJIbaLHpty5/hYDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"542e171cf3d60f08eb3c514b40730c63160ca871aba064985b7a5bcba5ef503d","last_reissued_at":"2026-07-05T09:11:26.782544Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:11:26.782544Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interacting holes in a gated WSe$_2$ quantum channel: valley correlations and zigzag Wigner crystal","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Adina Luican-Mayer, Daniel Miravet, Jaros{\\l}aw Paw{\\l}owski, Justin Boddison-Chouinard, Louis Gaudreau, Maciej Bieniek, Marek Korkusinski, Pawel Hawrylak","submitted_at":"2024-06-12T21:36:15Z","abstract_excerpt":"We present a theory of interacting valence holes in a gate-defined one-dimensional quantum channel in a single layer of a transition metal dichalcogenide material WSe$_2$. Based on a microscopic atomistic tight-binding model and Hartree-Fock and exact configuration-interaction tools we demonstrate the possibility of symmetry-broken valley polarized states for strongly interacting holes. The interplay between interactions, perpendicular magnetic field, and the lateral confinement asymmetry together with the strong Rashba spin-orbit coupling present in WSe$_2$ material is analyzed, and its impac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.08655","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/2406.08655/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":"2406.08655","created_at":"2026-07-05T09:11:26.782602+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.08655v2","created_at":"2026-07-05T09:11:26.782602+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.08655","created_at":"2026-07-05T09:11:26.782602+00:00"},{"alias_kind":"pith_short_12","alias_value":"KQXBOHHT2YHQ","created_at":"2026-07-05T09:11:26.782602+00:00"},{"alias_kind":"pith_short_16","alias_value":"KQXBOHHT2YHQR2Z4","created_at":"2026-07-05T09:11:26.782602+00:00"},{"alias_kind":"pith_short_8","alias_value":"KQXBOHHT","created_at":"2026-07-05T09:11:26.782602+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/KQXBOHHT2YHQR2Z4KFFUA4YMMM","json":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM.json","graph_json":"https://pith.science/api/pith-number/KQXBOHHT2YHQR2Z4KFFUA4YMMM/graph.json","events_json":"https://pith.science/api/pith-number/KQXBOHHT2YHQR2Z4KFFUA4YMMM/events.json","paper":"https://pith.science/paper/KQXBOHHT"},"agent_actions":{"view_html":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM","download_json":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM.json","view_paper":"https://pith.science/paper/KQXBOHHT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.08655&json=true","fetch_graph":"https://pith.science/api/pith-number/KQXBOHHT2YHQR2Z4KFFUA4YMMM/graph.json","fetch_events":"https://pith.science/api/pith-number/KQXBOHHT2YHQR2Z4KFFUA4YMMM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM/action/storage_attestation","attest_author":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM/action/author_attestation","sign_citation":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM/action/citation_signature","submit_replication":"https://pith.science/pith/KQXBOHHT2YHQR2Z4KFFUA4YMMM/action/replication_record"}},"created_at":"2026-07-05T09:11:26.782602+00:00","updated_at":"2026-07-05T09:11:26.782602+00:00"}