{"id":606744,"date":"2019-09-02T14:41:44","date_gmt":"2019-09-02T21:41:44","guid":{"rendered":"https:\/\/cm-edgetun.pages.dev\/en-us\/research\/?post_type=msr-research-item&#038;p=606744"},"modified":"2019-09-02T14:43:34","modified_gmt":"2019-09-02T21:43:34","slug":"the-role-of-entropy-in-topological-quantum-error-correction","status":"publish","type":"msr-research-item","link":"https:\/\/cm-edgetun.pages.dev\/en-us\/research\/publication\/the-role-of-entropy-in-topological-quantum-error-correction\/","title":{"rendered":"The role of entropy in topological quantum error correction"},"content":{"rendered":"<p>The performance of a quantum error-correction process is determined by the likelihood that a<br \/>\nrandom configuration of errors introduced to the system will lead to the corruption of encoded<br \/>\nlogical information. In this work we compare two different variants of the surface code with a<br \/>\ncomparable number of qubits: the surface code defined on a square lattice and the same model on a<br \/>\nlattice that is rotated by \u03c0\/4. This seemingly innocuous change increases the distance of the code<br \/>\nby a factor of \u221a2. However, as we show, this gain can come at the expense of significantly increasing<br \/>\nthe number of different failure mechanisms that are likely to occur. We use a number of different<br \/>\nmethods to explore this tradeoff over a large range of parameter space under an independent and<br \/>\nidentically distributed noise model. We rigorously analyze the leading order performance for low<br \/>\nerror rates, where the larger distance code performs best for all system sizes. Using an analytical<br \/>\nmodel and Monte Carlo sampling, we find that this improvement persists for fixed sub-threshold<br \/>\nerror rates for large system size, but that the improvement vanishes close to threshold. Remarkably,<br \/>\nintensive numerics uncover a region of system sizes and sub-threshold error rates where the square<br \/>\nlattice surface code marginally outperforms the rotated model.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The performance of a quantum error-correction process is determined by the likelihood that a random configuration of errors introduced to the system will lead to the corruption of encoded logical information. In this work we compare two different variants of the surface code with a comparable number of qubits: the surface code defined on a [&hellip;]<\/p>\n","protected":false},"featured_media":0,"template":"","meta":{"msr-url-field":"","msr-podcast-episode":"","msrModifiedDate":"","msrModifiedDateEnabled":false,"ep_exclude_from_search":false,"_classifai_error":"","msr-author-ordering":null,"msr_publishername":"","msr_publisher_other":"","msr_booktitle":"","msr_chapter":"","msr_edition":"","msr_editors":"","msr_how_published":"","msr_isbn":"","msr_issue":"","msr_journal":"Journal of Statistical Mechanics","msr_number":"","msr_organization":"","msr_pages_string":"","msr_page_range_start":"073404","msr_page_range_end":"","msr_series":"","msr_volume":"2019","msr_copyright":"","msr_conference_name":"","msr_doi":"","msr_arxiv_id":"","msr_s2_paper_id":"","msr_mag_id":"","msr_pubmed_id":"","msr_other_authors":"","msr_other_contributors":"","msr_speaker":"","msr_award":"","msr_affiliation":"","msr_institution":"","msr_host":"","msr_version":"","msr_duration":"","msr_original_fields_of_study":"","msr_release_tracker_id":"","msr_s2_match_type":"","msr_citation_count_updated":"","msr_published_date":"2019-7-18","msr_highlight_text":"","msr_notes":"","msr_longbiography":"","msr_publicationurl":"","msr_external_url":"","msr_secondary_video_url":"","msr_conference_url":"","msr_journal_url":"","msr_s2_pdf_url":"","msr_year":0,"msr_citation_count":0,"msr_influential_citations":0,"msr_reference_count":0,"msr_s2_match_confidence":0,"msr_microsoftintellectualproperty":true,"msr_s2_open_access":false,"msr_s2_author_ids":[],"msr_pub_ids":[],"msr_hide_image_in_river":0,"footnotes":""},"msr-research-highlight":[],"research-area":[243138],"msr-publication-type":[193715],"msr-publisher":[],"msr-focus-area":[],"msr-locale":[268875],"msr-post-option":[],"msr-field-of-study":[],"msr-conference":[],"msr-journal":[],"msr-impact-theme":[],"msr-pillar":[],"class_list":["post-606744","msr-research-item","type-msr-research-item","status-publish","hentry","msr-research-area-quantum","msr-locale-en_us"],"msr_publishername":"","msr_edition":"","msr_affiliation":"","msr_published_date":"2019-7-18","msr_host":"","msr_duration":"","msr_version":"","msr_speaker":"","msr_other_contributors":"","msr_booktitle":"","msr_pages_string":"","msr_chapter":"","msr_isbn":"","msr_journal":"Journal of Statistical Mechanics","msr_volume":"2019","msr_number":"","msr_editors":"","msr_series":"","msr_issue":"","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":"url","viewUrl":"false","id":"false","title":"https:\/\/arxiv.org\/pdf\/1812.05117.pdf","label_id":"243109","label":0}],"msr_related_uploader":"","msr_citation_count":0,"msr_citation_count_updated":"","msr_s2_paper_id":"","msr_influential_citations":0,"msr_reference_count":0,"msr_arxiv_id":"","msr_s2_author_ids":[],"msr_s2_open_access":false,"msr_s2_pdf_url":null,"msr_attachments":[],"msr-author-ordering":[{"type":"user_nicename","value":"Michael Beverland","user_id":36849,"rest_url":"https:\/\/cm-edgetun.pages.dev\/en-us\/research\/wp-json\/microsoft-research\/v1\/researchers?person=Michael Beverland"},{"type":"text","value":"Benjamin J. 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