{"id":426771,"date":"2018-11-06T16:57:18","date_gmt":"2018-11-07T00:57:18","guid":{"rendered":"https:\/\/www.microsoft.com\/en-us\/research\/?post_type=msr-research-item&#038;p=426771"},"modified":"2018-11-06T16:57:18","modified_gmt":"2018-11-07T00:57:18","slug":"exponential-lifetime-improvement-topological-quantum-memories","status":"publish","type":"msr-research-item","link":"https:\/\/www.microsoft.com\/en-us\/research\/publication\/exponential-lifetime-improvement-topological-quantum-memories\/","title":{"rendered":"Exponential Lifetime Improvement in Topological Quantum Memories"},"content":{"rendered":"<p>We propose a simple yet efficient mechanism for passive error correction in topological quantum memories. Our scheme relies on driven-dissipative ancilla systems which couple to local excitations (anyons) and make them &#8220;sink&#8221; in energy, with no required interaction among ancillae or anyons. Through this process, anyons created by some thermal environment end up trapped in potential &#8220;trenches&#8221; that they themselves generate, which can be interpreted as a &#8220;memory foam&#8221; for anyons. This self-trapping mechanism provides an energy barrier for anyon propagation, and removes entropy from the memory by favoring anyon recombination over anyon separation (responsible for memory errors). We demonstrate that our scheme leads to an exponential increase of the memory-coherence time with system size\u00a0<span id=\"MathJax-Element-1-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"mi\">L<\/span><\/span><\/span><\/span>, up to an upper bound\u00a0<span id=\"MathJax-Element-2-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-4\" class=\"math\"><span id=\"MathJax-Span-5\" class=\"mrow\"><span id=\"MathJax-Span-6\" class=\"msubsup\"><span id=\"MathJax-Span-7\" class=\"mi\">L<\/span><span id=\"MathJax-Span-8\" class=\"texatom\"><span id=\"MathJax-Span-9\" class=\"mrow\"><span id=\"MathJax-Span-10\" class=\"mi\">m<\/span><span id=\"MathJax-Span-11\" class=\"mi\">a<\/span><span id=\"MathJax-Span-12\" class=\"mi\">x<\/span><\/span><\/span><\/span><\/span><\/span><\/span>\u00a0which can increase exponentially with\u00a0<span id=\"MathJax-Element-3-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-13\" class=\"math\"><span id=\"MathJax-Span-14\" class=\"mrow\"><span id=\"MathJax-Span-15\" class=\"mi\">\u0394<\/span><span id=\"MathJax-Span-16\" class=\"texatom\"><span id=\"MathJax-Span-17\" class=\"mrow\"><span id=\"MathJax-Span-18\" class=\"mo\">\/<\/span><\/span><\/span><span id=\"MathJax-Span-19\" class=\"mi\">T<\/span><\/span><\/span><\/span>, where\u00a0<span id=\"MathJax-Element-4-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-20\" class=\"math\"><span id=\"MathJax-Span-21\" class=\"mrow\"><span id=\"MathJax-Span-22\" class=\"mi\">T<\/span><\/span><\/span><\/span>\u00a0is the temperature and\u00a0<span id=\"MathJax-Element-5-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-23\" class=\"math\"><span id=\"MathJax-Span-24\" class=\"mrow\"><span id=\"MathJax-Span-25\" class=\"mi\">\u0394<\/span><\/span><\/span><\/span>\u00a0is some energy scale defined by potential trenches. This results in a double exponential increase of the memory time with\u00a0<span id=\"MathJax-Element-6-Frame\" class=\"MathJax\"><span id=\"MathJax-Span-26\" class=\"math\"><span id=\"MathJax-Span-27\" class=\"mrow\"><span id=\"MathJax-Span-28\" class=\"mi\">\u0394<\/span><span id=\"MathJax-Span-29\" class=\"texatom\"><span id=\"MathJax-Span-30\" class=\"mrow\"><span id=\"MathJax-Span-31\" class=\"mo\">\/<\/span><\/span><\/span><span id=\"MathJax-Span-32\" class=\"mi\">T<\/span><\/span><\/span><\/span>, which greatly improves over the Arrhenius (single-exponential) scaling found in typical quantum memories.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We propose a simple yet efficient mechanism for passive error correction in topological quantum memories. Our scheme relies on driven-dissipative ancilla systems which couple to local excitations (anyons) and make them &#8220;sink&#8221; in energy, with no required interaction among ancillae or anyons. Through this process, anyons created by some thermal environment end up trapped in [&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":"tokarzig"}],"msr_publishername":"","msr_publisher_other":"","msr_booktitle":"","msr_chapter":"","msr_edition":"","msr_editors":"","msr_how_published":"","msr_isbn":"","msr_issue":"","msr_journal":"Physical Review 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