{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:F2ZJYGJT34ABHSCSLSU7UKYXUB","short_pith_number":"pith:F2ZJYGJT","schema_version":"1.0","canonical_sha256":"2eb29c1933df0013c8525ca9fa2b17a0565c47e593455648ef0e3f301cd9637f","source":{"kind":"arxiv","id":"1302.2670","version":2},"attestation_state":"computed","paper":{"title":"Equilibration of quantum Hall edge states by an Ohmic contact","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Artur O. Slobodeniuk, Eugene V. Sukhorukov, Ivan P. Levkivskyi","submitted_at":"2013-02-11T23:55:05Z","abstract_excerpt":"Ohmic contacts are crucial elements of electron optics that have not received a clear theoretical description yet. We propose a model of an Ohmic contact as a piece of metal of the finite capacitance $C$ attached to a quantum Hall edge. It is shown that charged quantum Hall edge states may have weak coupling to neutral excitations in an Ohmic contact. Consequently, despite being a reservoir of neutral excitations, an Ohmic contact is not able to efficiently equilibrate edge states if its temperature is smaller than $\\hbar\\Omega_c$, where $\\Omega_c$ is the inverse RC time of the contact. This 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":"1302.2670","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-02-11T23:55:05Z","cross_cats_sorted":[],"title_canon_sha256":"4889c43b9c2b1855eb926540cada5dd3ea4a2feddb5bba3cc5d7e00285487c4d","abstract_canon_sha256":"0fcdc560644d2ebfd3917af21cf792ebeae95c4a187134f27ff83fa5184e0b33"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:42.379843Z","signature_b64":"JyUY/JbOHLEAV+oye9gDrR7BoXHNPOiBs0neyYgCEgBWOb8cT8yG62VVH78TStChamxg6euSmkGsm7a0evz2Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2eb29c1933df0013c8525ca9fa2b17a0565c47e593455648ef0e3f301cd9637f","last_reissued_at":"2026-05-18T01:51:42.379182Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:42.379182Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Equilibration of quantum Hall edge states by an Ohmic contact","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Artur O. Slobodeniuk, Eugene V. Sukhorukov, Ivan P. Levkivskyi","submitted_at":"2013-02-11T23:55:05Z","abstract_excerpt":"Ohmic contacts are crucial elements of electron optics that have not received a clear theoretical description yet. We propose a model of an Ohmic contact as a piece of metal of the finite capacitance $C$ attached to a quantum Hall edge. It is shown that charged quantum Hall edge states may have weak coupling to neutral excitations in an Ohmic contact. Consequently, despite being a reservoir of neutral excitations, an Ohmic contact is not able to efficiently equilibrate edge states if its temperature is smaller than $\\hbar\\Omega_c$, where $\\Omega_c$ is the inverse RC time of the contact. This e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.2670","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":"1302.2670","created_at":"2026-05-18T01:51:42.379293+00:00"},{"alias_kind":"arxiv_version","alias_value":"1302.2670v2","created_at":"2026-05-18T01:51:42.379293+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.2670","created_at":"2026-05-18T01:51:42.379293+00:00"},{"alias_kind":"pith_short_12","alias_value":"F2ZJYGJT34AB","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"F2ZJYGJT34ABHSCS","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"F2ZJYGJT","created_at":"2026-05-18T12:27:43.054852+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/F2ZJYGJT34ABHSCSLSU7UKYXUB","json":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB.json","graph_json":"https://pith.science/api/pith-number/F2ZJYGJT34ABHSCSLSU7UKYXUB/graph.json","events_json":"https://pith.science/api/pith-number/F2ZJYGJT34ABHSCSLSU7UKYXUB/events.json","paper":"https://pith.science/paper/F2ZJYGJT"},"agent_actions":{"view_html":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB","download_json":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB.json","view_paper":"https://pith.science/paper/F2ZJYGJT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1302.2670&json=true","fetch_graph":"https://pith.science/api/pith-number/F2ZJYGJT34ABHSCSLSU7UKYXUB/graph.json","fetch_events":"https://pith.science/api/pith-number/F2ZJYGJT34ABHSCSLSU7UKYXUB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB/action/storage_attestation","attest_author":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB/action/author_attestation","sign_citation":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB/action/citation_signature","submit_replication":"https://pith.science/pith/F2ZJYGJT34ABHSCSLSU7UKYXUB/action/replication_record"}},"created_at":"2026-05-18T01:51:42.379293+00:00","updated_at":"2026-05-18T01:51:42.379293+00:00"}