{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:YPCXTBUL4YOI5ZBIIGNRP6RKXM","short_pith_number":"pith:YPCXTBUL","schema_version":"1.0","canonical_sha256":"c3c579868be61c8ee428419b17fa2abb1afb0f21741e24f332a1918cbc094d83","source":{"kind":"arxiv","id":"cond-mat/9909096","version":2},"attestation_state":"computed","paper":{"title":"Edge Modes Waves in Superlattices in Quantum Hall Effect Regime","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alejandro Cabo Montes de Oca, Carlos Rodriguez Castellanos, Pavel Fileviez Perez","submitted_at":"1999-09-07T01:12:19Z","abstract_excerpt":"The wave propagation of edge modes in a superlattice of 2D electron Gases in quantum Hall regime is investigated. After introducing surfaces charge and current densities at the edge, the Maxwell equations are solved for waves running along the boundary. The constitutive relations expressing the edge charge and current densities in terms of the fields at the boundary are derived. One of them is similar to the London equation for superconductor currents. The dispersion relation and wave polarizations for the momenta region $w/c<k$ are also obtained for propagation along the borderlines of the el"},"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":"cond-mat/9909096","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"1999-09-07T01:12:19Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a4c08c1acc2d8fd966d450458a950936a5eb16eb6db53b816bc2ae96963df021","abstract_canon_sha256":"5062e361e4e8f235024f9641508a7d60c79932e9e3143a1152503420244681f6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:27.349992Z","signature_b64":"IaNHyCv/4qSpC0UTJC1RH2mkG9p2/RW0gwkDV+mSmUSl+Me5tHxiQ3C+rBqaJQhBxeAvj4j6d3WO7CBOtxjaCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3c579868be61c8ee428419b17fa2abb1afb0f21741e24f332a1918cbc094d83","last_reissued_at":"2026-05-18T01:39:27.349581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:27.349581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Edge Modes Waves in Superlattices in Quantum Hall Effect Regime","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alejandro Cabo Montes de Oca, Carlos Rodriguez Castellanos, Pavel Fileviez Perez","submitted_at":"1999-09-07T01:12:19Z","abstract_excerpt":"The wave propagation of edge modes in a superlattice of 2D electron Gases in quantum Hall regime is investigated. After introducing surfaces charge and current densities at the edge, the Maxwell equations are solved for waves running along the boundary. The constitutive relations expressing the edge charge and current densities in terms of the fields at the boundary are derived. One of them is similar to the London equation for superconductor currents. The dispersion relation and wave polarizations for the momenta region $w/c<k$ are also obtained for propagation along the borderlines of the el"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9909096","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":""},"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":"cond-mat/9909096","created_at":"2026-05-18T01:39:27.349636+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9909096v2","created_at":"2026-05-18T01:39:27.349636+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9909096","created_at":"2026-05-18T01:39:27.349636+00:00"},{"alias_kind":"pith_short_12","alias_value":"YPCXTBUL4YOI","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"YPCXTBUL4YOI5ZBI","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"YPCXTBUL","created_at":"2026-05-18T12:25:49.631198+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/YPCXTBUL4YOI5ZBIIGNRP6RKXM","json":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM.json","graph_json":"https://pith.science/api/pith-number/YPCXTBUL4YOI5ZBIIGNRP6RKXM/graph.json","events_json":"https://pith.science/api/pith-number/YPCXTBUL4YOI5ZBIIGNRP6RKXM/events.json","paper":"https://pith.science/paper/YPCXTBUL"},"agent_actions":{"view_html":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM","download_json":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM.json","view_paper":"https://pith.science/paper/YPCXTBUL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9909096&json=true","fetch_graph":"https://pith.science/api/pith-number/YPCXTBUL4YOI5ZBIIGNRP6RKXM/graph.json","fetch_events":"https://pith.science/api/pith-number/YPCXTBUL4YOI5ZBIIGNRP6RKXM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM/action/storage_attestation","attest_author":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM/action/author_attestation","sign_citation":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM/action/citation_signature","submit_replication":"https://pith.science/pith/YPCXTBUL4YOI5ZBIIGNRP6RKXM/action/replication_record"}},"created_at":"2026-05-18T01:39:27.349636+00:00","updated_at":"2026-05-18T01:39:27.349636+00:00"}