{"id":719563,"date":"2021-01-22T09:12:14","date_gmt":"2021-01-22T17:12:14","guid":{"rendered":"https:\/\/www.microsoft.com\/en-us\/research\/?post_type=msr-research-item&p=719563"},"modified":"2021-01-22T09:12:14","modified_gmt":"2021-01-22T17:12:14","slug":"repairing-the-surface-of-inas-based-topological-heterostructures","status":"publish","type":"msr-research-item","link":"https:\/\/www.microsoft.com\/en-us\/research\/publication\/repairing-the-surface-of-inas-based-topological-heterostructures\/","title":{"rendered":"Repairing the surface of InAs-based topological heterostructures"},"content":{"rendered":"

Candidate systems for topologically-protected qubits include two-dimensional electron gases (2DEGs) based on heterostructures exhibiting a strong spin\u2013orbit interaction and superconductivity via the proximity effect. For InAs- or InSb-based materials, the need to form shallow quantum wells to create a hard-gapped p-wave superconducting state often subjects them to fabrication-induced damage, limiting their mobility. Here, we examine scattering mechanisms in processed InAs 2DEG quantum wells and demonstrate a means of increasing their mobility via repairing the semiconductor\u2013dielectric interface. Passivation of charged impurity states with an argon\u2013hydrogen plasma results in a significant increase in the measured mobility and reduction in its variance relative to untreated samples, up to 45\u2009300\u2009cm 2\/(V\u2009s) in a 10\u2009nm deep quantum well.<\/p>\n","protected":false},"excerpt":{"rendered":"

Candidate systems for topologically-protected qubits include two-dimensional electron gases (2DEGs) based on heterostructures exhibiting a strong spin\u2013orbit interaction and superconductivity via the proximity effect. For InAs- or InSb-based materials, the need to form shallow quantum wells to create a hard-gapped p-wave superconducting state often subjects them to fabrication-induced damage, limiting their mobility. Here, we examine […]<\/p>\n","protected":false},"featured_media":0,"template":"","meta":{"msr-url-field":"","msr-podcast-episode":"","msrModifiedDate":"","msrModifiedDateEnabled":false,"ep_exclude_from_search":false,"footnotes":""},"msr-content-type":[3],"msr-research-highlight":[],"research-area":[243138],"msr-publication-type":[193715],"msr-product-type":[],"msr-focus-area":[],"msr-platform":[],"msr-download-source":[],"msr-locale":[268875],"msr-field-of-study":[249709,249733,249286,247912,249277,250144,249289,249370,249772,249292],"msr-conference":[],"msr-journal":[],"msr-impact-theme":[],"msr-pillar":[],"class_list":["post-719563","msr-research-item","type-msr-research-item","status-publish","hentry","msr-research-area-quantum","msr-locale-en_us","msr-field-of-study-condensed-matter-physics","msr-field-of-study-electron","msr-field-of-study-heterojunction","msr-field-of-study-materials-science","msr-field-of-study-passivation","msr-field-of-study-proximity-effect-audio","msr-field-of-study-quantum-well","msr-field-of-study-qubit","msr-field-of-study-scattering","msr-field-of-study-superconductivity"],"msr_publishername":"","msr_edition":"","msr_affiliation":"","msr_published_date":"2020-9-14","msr_host":"","msr_duration":"","msr_version":"","msr_speaker":"","msr_other_contributors":"","msr_booktitle":"","msr_pages_string":"","msr_chapter":"","msr_isbn":"","msr_journal":"Journal of Applied Physics","msr_volume":"128","msr_number":"","msr_editors":"","msr_series":"","msr_issue":"11","msr_organization":"","msr_how_published":"","msr_notes":"","msr_highlight_text":"","msr_release_tracker_id":"","msr_original_fields_of_study":"","msr_download_urls":"","msr_external_url":"","msr_secondary_video_url":"","msr_longbiography":"","msr_microsoftintellectualproperty":1,"msr_main_download":"","msr_publicationurl":"","msr_doi":"","msr_publication_uploader":[{"type":"doi","viewUrl":"false","id":"false","title":"10.1063\/5.0014361","label_id":"243106","label":0}],"msr_related_uploader":"","msr_attachments":[],"msr-author-ordering":[{"type":"text","value":"S. J. Pauka","user_id":0,"rest_url":false},{"type":"text","value":"J. D. S. Witt","user_id":0,"rest_url":false},{"type":"text","value":"C. N. Allen","user_id":0,"rest_url":false},{"type":"text","value":"B. Harlech-Jones","user_id":0,"rest_url":false},{"type":"text","value":"A. Jouan","user_id":0,"rest_url":false},{"type":"user_nicename","value":"Geoff Gardner","user_id":36825,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=Geoff Gardner"},{"type":"user_nicename","value":"Sergei Gronin","user_id":36927,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=Sergei Gronin"},{"type":"text","value":"T. Wang","user_id":0,"rest_url":false},{"type":"text","value":"C. Thomas","user_id":0,"rest_url":false},{"type":"guest","value":"professor-michael-j-manfra","user_id":425307,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=professor-michael-j-manfra"},{"type":"user_nicename","value":"Jan Gukelberger","user_id":36918,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=Jan Gukelberger"},{"type":"user_nicename","value":"John Gamble","user_id":37911,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=John Gamble"},{"type":"user_nicename","value":"David Reilly","user_id":36816,"rest_url":"https:\/\/www.microsoft.com\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=David Reilly"},{"type":"text","value":"M. C. 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