0:00:03 | one of the main questions in the class community is to understand how score of |
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0:00:07 | the or equivalently the relaxation time and temperature and density |
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0:00:12 | during the last ten years people are shown in simulations and experiments that instantly the |
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0:00:18 | relaxation fact that and one variable named density based to some materials is difficult and |
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0:00:24 | divided by virtue |
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0:00:27 | in this article we show our simulations and experiments that the last density variation |
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0:00:32 | this variable can not you describe entire face diagram |
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0:00:37 | similarly three icicle this |
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0:00:40 | one point two one point six and two point zero applying the relaxation target densities |
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0:00:46 | giving verbal with two different choices are gonna |
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0:00:49 | it is clear that one thing the canonical or icicles |
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0:00:54 | in order to explain this we use a new cluster two thousand and nine in |
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0:00:58 | statistical mechanics score are small |
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0:01:01 | to they want to define be isomorphic yes of my configurations have proposed configuration of |
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0:01:08 | all vectors |
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0:01:10 | from this alone can be shown that the relaxation time based more formal fading name |
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0:01:16 | the skating variable is a function of the city divided but image |
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0:01:21 | prediction of ice able you re is that i think i didn't structure and dynamics |
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0:01:28 | we illustrate this by showing simulations three state but two of them are isomorphic and |
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0:01:34 | that there is not |
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0:01:36 | the first one is that a separate u and low density |
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0:01:40 | and we visualize the position of excess it's very old and probably structure instantaneously by |
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0:01:46 | calculating the radio distribution function |
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0:01:49 | seen in the lower panel |
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0:01:51 | recent similar to keep intensity constant which she does not change significantly |
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0:01:57 | poking yes |
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0:01:59 | now changing density and temperature so that they are isomorphic with this one with either |
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0:02:06 | except the thing structure this despite this is increased by more than sixty percent |
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0:02:13 | now that you small ravenous we apply the same data as shown in figure one |
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0:02:17 | and c you could collect for icicles |
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0:02:21 | so conclusion we have shown that power densities getting breakdown last density variations |
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0:02:27 | we propose musically variable derived from the i-th small theory and verified via |
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0:02:33 | simulations one it's missing boundary |
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0:02:37 | model which is the data we have just see |
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0:02:39 | we also data from simulations to model molecular liquids |
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0:02:44 | and present data from two you spend about |
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0:02:48 | or confirming the proposal at the re |
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0:02:51 | with this game where we use face to one dimensions |
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0:02:57 | thank you for which |
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