{"id":165719,"date":"2018-11-06T17:21:51","date_gmt":"2018-11-07T01:21:51","guid":{"rendered":"https:\/\/www.microsoft.com\/en-us\/research\/msr-research-item\/asymptotically-optimal-topological-quantum-compiling\/"},"modified":"2018-11-06T17:21:51","modified_gmt":"2018-11-07T01:21:51","slug":"asymptotically-optimal-topological-quantum-compiling","status":"publish","type":"msr-research-item","link":"https:\/\/www.microsoft.com\/en-us\/research\/publication\/asymptotically-optimal-topological-quantum-compiling\/","title":{"rendered":"Asymptotically Optimal Topological Quantum Compiling"},"content":{"rendered":"<div class=\"asset-content\">\n<p>We address the problem of compiling quantum operations into braid representations for non-Abelian quasiparticles described by the Fibonacci anyon model. We classify the single-qubit unitaries that can be represented exactly by Fibonacci anyon braids and use the classification to develop a probabilistically polynomial algorithm that approximates any given single-qubit unitary to a desired precision by an asymptotically depth-optimal braid pattern. We extend our algorithm in two directions: to produce braids that allow only single-strand movement, called weaves, and to produce depth-optimal approximations of two-qubit gates. Our compiled braid patterns have depths that are 20 to 1000 times shorter than those output by prior state-of-the-art methods, for precisions ranging between <span class=\"aps-inline-formula\"><span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"mrow\"><span id=\"MathJax-Span-4\" class=\"mn\">1<\/span><span id=\"MathJax-Span-5\" class=\"msup\"><span id=\"MathJax-Span-6\" class=\"mrow\"><span id=\"MathJax-Span-7\" class=\"mn\">0<\/span><\/span><span id=\"MathJax-Span-8\" class=\"mrow\"><span id=\"MathJax-Span-9\" class=\"mo\">\u2212<\/span><span id=\"MathJax-Span-10\" class=\"mn\">10<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span> and <span class=\"aps-inline-formula\"><span id=\"MathJax-Element-2-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-11\" class=\"math\"><span id=\"MathJax-Span-12\" class=\"mrow\"><span id=\"MathJax-Span-13\" class=\"mn\">1<\/span><span id=\"MathJax-Span-14\" class=\"msup\"><span id=\"MathJax-Span-15\" class=\"mn\">0<\/span><span id=\"MathJax-Span-16\" class=\"mrow\"><span id=\"MathJax-Span-17\" class=\"mo\">\u2212<\/span><span id=\"MathJax-Span-18\" class=\"mn\">30<\/span><\/span><\/span><\/span><\/span><\/span><\/span>.<\/p>\n<\/div>\n<p><!-- .asset-content --><\/p>\n","protected":false},"excerpt":{"rendered":"<p>We address the problem of compiling quantum operations into braid representations for non-Abelian quasiparticles described by the Fibonacci anyon model. We classify the single-qubit unitaries that can be represented exactly by Fibonacci anyon braids and use the classification to develop a probabilistically polynomial algorithm that approximates any given single-qubit unitary to a desired precision by [&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":[{"type":"user_nicename","value":"vadym","user_id":"34468"},{"type":"user_nicename","value":"alexeib","user_id":"30935"},{"type":"user_nicename","value":"ksvore","user_id":"32588"}],"msr_publishername":"APS","msr_publisher_other":"","msr_booktitle":"","msr_chapter":"","msr_edition":"","msr_editors":"","msr_how_published":"","msr_isbn":"","msr_issue":"","msr_journal":"Physical Review Letters","msr_number":"","msr_organization":"","msr_pages_string":"","msr_page_range_start":"","msr_page_range_end":"","msr_series":"","msr_volume":"112","msr_copyright":"","msr_conference_name":"","msr_doi":"10.1103\/PhysRevLett.112.140504","msr_arxiv_id":"","msr_s2_paper_id":"","msr_mag_id":"","msr_pubmed_id":"","msr_other_authors":"Krysta M. 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