0:00:03 | de mining is sign invention |
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0:00:06 | together with my colleague in a sense of the quantum technologies in singapore i've been |
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0:00:11 | thinking about particular approach to a building |
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0:00:15 | quantum computers |
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0:00:16 | with both there is so what we do is what task on paper and hope |
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0:00:19 | it is interesting to the experiments as |
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0:00:22 | but i love a paper is high threshold |
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0:00:25 | distributed quantum computing with three two bit nodes just quite an awful i think it |
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0:00:30 | by explain what that means all of done a pretty stable job of explaining |
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0:00:35 | okay |
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0:00:36 | so on some computers of course of a stream of modern physics the idea of |
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0:00:40 | the machine that harnesses quantum states in order to do calculations there are |
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0:00:45 | effectively impossible with ordinary technology |
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0:00:49 | in order to build such machine we need to have a very large number of |
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0:00:52 | components each of which is stored in quantum state so that be the basic components |
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0:00:56 | is that you that we need lots of them |
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0:00:58 | or under good control |
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0:01:01 | be distributed quantum computing approach is kind of an architectural overall scheme have to do |
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0:01:07 | this |
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0:01:07 | which tries to make things a scalable as possible |
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0:01:10 | so the idea is don't put only a few bits into a single grand or |
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0:01:14 | a monolithic structure that is one week ago but |
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0:01:17 | in this t v two q i p instead you try and build small units |
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0:01:22 | which michael more tools pornos each of which has only a few bits inside it |
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0:01:27 | you get to the building that's and controlling it and you make lots of them |
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0:01:30 | and welcome to get to make the last machine the network you expect to the |
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0:01:35 | and we see that work for network |
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0:01:37 | and that's actual scheme for the entire machine it's distributed in the sense that it's |
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0:01:41 | kind of exploded out from a single monolithic structure but of course not distributed over |
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0:01:46 | large distances in one room |
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0:01:48 | okay so that but thresholding |
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0:01:51 | okay so a threshold in the u refers to |
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0:01:56 | a level of precision that you need to reach in order that when you trying |
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0:02:00 | to a large scale computation the errors don't get out of control instead the arrows |
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0:02:04 | are coming in at low enough rate that you can detect and correct and for |
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0:02:09 | that basically if you're |
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0:02:12 | within your threshold you can do this outside of the threshold and errors will build |
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0:02:16 | up so fast that the calculation goes off track and get you know |
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0:02:19 | so of course you want a threshold the bs the mystic as possible as high |
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0:02:23 | as possible |
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0:02:25 | what you know like what's also this let's try and figure out what is the |
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0:02:29 | threshold for this distribute a quantum computing approach we're gonna have to keep numbers how |
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0:02:34 | it is the network okay just a controlled inside the node and we can also |
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0:02:38 | only three cue but spend a week or about that case "'cause" we put it |
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0:02:42 | would be the simplest case that would give us |
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0:02:45 | a good threshold |
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0:02:47 | three people nodes are reasonable thing to ask for lots of experimental groups can basically |
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0:02:51 | do that can basically q three q s |
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0:02:54 | so what we found was |
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0:02:56 | that we a partial was |
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0:02:58 | ten percent noise in the network which means one time and ten |
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0:03:02 | when you try and communicative network it just on bananas the you across to keep |
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0:03:06 | it simple |
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0:03:07 | and no point one percent noise with in the nodes themselves that means |
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0:03:13 | on those rare occasions when you try and the human or something it actually correct |
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0:03:17 | that q so |
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0:03:18 | ten percent of the network what one percent for the |
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0:03:22 | local operations in each that |
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0:03:24 | but as numbers are time especially the ninety nine point nine percent precision within each |
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0:03:28 | node star |
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0:03:29 | but not ridiculously so there are experimental groups in a syntactic units or in |
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0:03:35 | all tracks lindy sentences were pushing past sort of ninety nine percent threshold so |
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0:03:41 | that could be rich but also we stress that we have with trying to improve |
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0:03:45 | this point back to schemes that have |
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0:03:47 | even more optimistic specials |
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0:03:49 | you know the same time as the experiments is trying to improve |
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0:03:52 | their stuff and |
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0:03:53 | we have that soon not and you know pretty soon |
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0:03:55 | we may see these numbers actually meeting and then in principle you do we are |
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0:03:59 | trying to |
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0:04:01 | a large-scale machine |
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0:04:02 | okay so a few remarks the experts a how do we get a high threshold |
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0:04:07 | with such a small number keep a node we basically a and in something which |
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0:04:11 | is pretty much most of the previous role as a done which is to distill |
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0:04:15 | well as within each node |
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0:04:16 | a high quality and use those two power actual once again between local units |
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0:04:21 | your client of data humans we don't do that instead we currently project no easy |
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0:04:26 | hardy projections on the core units we do that repeated the until the party projection |
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0:04:31 | becomes |
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0:04:32 | effectively your and it's the resulting to o can go from a while back but |
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0:04:36 | it's basically can be done |
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0:04:38 | so then we just use the art objections to make some useful what we may |
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0:04:41 | is the three d cost the state of which is a resource for a topological |
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0:04:46 | quantum computing in the start described by prosody |
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0:04:50 | so that's okay and we find we only six party projections to do it which |
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0:04:54 | is basically why we're able to guess i threshold |
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0:04:58 | okay what if any if any of this it is of interest reading the papers |
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0:05:01 | of interest please don't hesitate to our contact me |
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0:05:04 | comments criticisms |
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