0:00:05 | the strange down to in the background |
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0:00:07 | we hesitate column |
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0:00:11 | represent mathematics |
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0:00:13 | whose acoustic training about this paper on be modeled area quite sure is about |
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0:00:19 | i score here in random matrices random way |
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0:00:23 | the context of the observation visual perception if you have some acoustic spectrum a century |
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0:00:30 | ago with those of today one difference you met you know this is what papers |
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0:00:35 | contain many more pictures |
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0:00:37 | there are two reasons for this purpose is a growing recognition one equation is a |
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0:00:42 | compact summary complex idea is very compact estimate how to appreciate |
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0:00:47 | and i really worth of that words can help us classes content |
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0:00:53 | the second reason is with one software is quick and easy to make pictures rich |
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0:00:59 | information |
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0:01:01 | by contrast whether we have you representations of mathematics asylums absence of hearing is not |
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0:01:07 | in systematically investigated as a guide the conventional mathematical concepts |
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0:01:13 | our drinks represent two areas of mathematical physics |
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0:01:17 | the first area is random matrix theory this way of characterizing energy levels in quantum |
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0:01:24 | system technology that's study quantum systems with classical counterpart of the scale or |
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0:01:32 | more generally characterized is |
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0:01:34 | i mean values some mathematical property of operations systems vibration the conjugate |
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0:01:41 | random actually they represent condition was and captures the statistics |
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0:01:47 | there are three nine types of randomly statistics different fluctuation properties related to the symmetry |
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0:01:54 | of the underlying dynamics and the purpose of this study was to find out the |
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0:01:58 | differences can be |
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0:02:00 | to this is necessary to run to the interval sequences there are many ways to |
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0:02:06 | do this one but we are in the paper integrate functions of zeros at the |
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0:02:12 | end of this there are many possibilities |
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0:02:15 | we find rendering functions as high modulation carrier waves could be |
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0:02:21 | the rest sets of so that several that's each lasting used in set consists of |
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0:02:27 | five clicks the three random vector function somewhere between a function representing the original was |
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0:02:34 | one represents all ninety completely uncorrelated random |
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0:02:39 | also industry |
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0:02:42 | no way we represent cell great sequences from the mean do not correspond to the |
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0:02:48 | spacing between adjacent okay differences between the types of random matrix can be distinguished by |
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0:02:55 | this |
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0:02:56 | the second there that we had a random way into three dimensions |
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0:03:02 | these are right but i think anymore automatically extracting in different directions representing for example |
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0:03:08 | laces spectral black body radiation the bayesian inverse quantum electron waves chaotic quantum dots |
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0:03:16 | many examples random way |
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0:03:20 | one dimensional sections such as a function of a single position where and efficient way |
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0:03:25 | to this time |
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0:03:26 | the sections can be rented sounds that every again as phase modulated carrier where the |
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0:03:32 | point was that the equation |
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0:03:34 | in two and three dimensions and be distinguished represented in this way |
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0:03:41 | we are not experts in sampras and we got this type as the total in |
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0:03:46 | the beginning |
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0:03:47 | further developments come quickly to mark |
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0:03:49 | more sophisticated renderings for example involving rhythm how many and number as well as pitch |
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0:03:55 | as we can clearly introduction |
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0:03:57 | this paper is currently speculative |
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0:04:00 | where the mathematics |
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0:04:01 | is useful or major curiosity remains to be seen |
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0:04:05 | or rather |
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