0:00:10 | one the key problems |
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0:00:12 | you'll be reading about |
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0:00:14 | in this special issue on a topological quantum computing |
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0:00:18 | is known to extract information which were hidden inside a total articulate |
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0:00:27 | you don't look you behind the information from the environment |
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0:00:31 | and that intensity information from the coherence |
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0:00:35 | but this very same property |
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0:00:37 | makes it very difficult to extract information once you needed |
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0:00:42 | this is the major problem |
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0:00:44 | and in this work |
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0:00:46 | we go one way around |
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0:00:53 | this is a proposal |
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0:00:55 | to use the flux to read to read out the state of the topological q |
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0:00:59 | but |
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0:01:00 | welcome back to this device in just a moment |
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0:01:03 | let me first walk you through the basic mechanism |
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0:01:07 | the topological cube it consists of |
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0:01:10 | ward distance |
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0:01:12 | in a super conductor |
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0:01:14 | and together these two voices encode the state different you |
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0:01:19 | they do this in such a way that the state of the cube it is |
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0:01:22 | protected from perturbations asking only on one of the |
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0:01:26 | basically the state of the cubic zero if the party of the number of elections |
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0:01:31 | in the superconducting i don't even |
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0:01:34 | and the state is one |
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0:01:35 | the better results |
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0:01:37 | no you would like to read out the state |
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0:01:39 | without actually counting the elections |
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0:01:42 | and the way to do this is to the fact call the |
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0:01:44 | however cash effect |
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0:01:48 | i perfect states |
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0:01:50 | then be more cakes encircling superconducting either |
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0:01:55 | would be classification |
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0:01:57 | which is determined by the parity of the number of particles |
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0:02:01 | inside the i don't |
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0:02:04 | this looks good |
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0:02:06 | but there is a problem with this effect |
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0:02:08 | which is that i mean cost of work is to switch |
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0:02:12 | or differences which are used to define a topological humans |
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0:02:16 | these are massive classical objects |
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0:02:19 | they do not interfere |
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0:02:22 | so this would not work |
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0:02:24 | our proposal is to work around this |
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0:02:27 | by using another type of forty six |
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0:02:30 | which have no for |
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0:02:32 | it is the normal core of the because for texas |
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0:02:35 | basically this whole superconducting |
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0:02:38 | which makes the mess |
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0:02:40 | so we would like to use corners boxes |
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0:02:43 | these exist "'cause" shows a simple pieces and eleven injunction joe's injunction which is just |
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0:02:49 | a tunnel battery across the superconducting |
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0:02:52 | and the chosen for this is will address along the tunnel junction |
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0:02:56 | some of the superconducting i don't |
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0:03:00 | ending because of what pieces and thereby measured already |
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0:03:04 | of number of the lectures and read out that a large document |
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0:03:09 | no the device which we propose is a hybrid devices |
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0:03:13 | it consists of a superconducting bring |
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0:03:16 | this is the flux you met |
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0:03:18 | according to superconducting drinkers little clockwise |
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0:03:21 | what counterclockwise |
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0:03:24 | and its interface with a topological cute |
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0:03:28 | in this particular we get a station the role of because the forties this is |
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0:03:31 | clearly time domain blocks |
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0:03:34 | your |
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0:03:36 | and you more select one |
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0:03:39 | so here we have a hybrid system consisting of a topological q but these |
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0:03:44 | white dots which store |
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0:03:46 | one of them information in a way which is topological protected |
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0:03:50 | and the momel documents |
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0:03:52 | which is able to provide computed by the time of crusher effect |
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0:03:56 | and thereby can be out the state of the stuff like to compute |
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0:04:01 | so this is a device which |
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0:04:03 | we hope |
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0:04:04 | combines the best of both worlds |
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0:04:06 | the ease with which class to which is a conventional q but can be read |
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0:04:10 | out |
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0:04:11 | and the protection against incoherence from the environment |
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0:04:14 | which is offered by topological q |
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