0:00:03 | welcome to all work on guaranteed global synchronisation networks were stochastic interaction |
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0:00:10 | synchronization is that it in various view that shared by all the two |
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0:00:14 | you think |
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0:00:15 | and engineering |
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0:00:16 | right on the one inside you might have |
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0:00:19 | continuous coupling |
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0:00:21 | you might have on the other hand side this continuous part company |
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0:00:26 | especially in the field of wireless communication |
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0:00:29 | where packets are transmitted |
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0:00:32 | and receive |
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0:00:34 | quite naturally a discontinuous system |
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0:00:37 | so you're interested in parts coupling |
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0:00:40 | at the strategy to |
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0:00:42 | achieve synchronization |
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0:00:45 | with that just to them |
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0:00:46 | you might have |
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0:00:48 | i which are net the conditions |
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0:00:50 | and individual delay and additionally you will have a probability to read the packet |
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0:01:00 | this mean |
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0:01:01 | that |
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0:01:02 | there is a chance |
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0:01:04 | then the signal that is transmitted is not going to be written |
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0:01:08 | the that's all the to be taken into account |
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0:01:11 | if you want to achieve and guarantee think annotation |
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0:01:15 | and that's exactly what we do |
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0:01:17 | and i'm going to show you now how we going to achieve this goal |
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0:01:24 | let us take |
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0:01:27 | late the running |
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0:01:28 | on a circle |
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0:01:30 | here's the all clear |
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0:01:32 | entrance counterclockwise on the circle until it passes the threshold |
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0:01:37 | whenever tested a threshold |
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0:01:39 | it will emitted signal |
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0:01:41 | with some probability |
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0:01:44 | p ten |
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0:01:45 | any oscillator |
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0:01:47 | on the circle which receives the signal |
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0:01:50 | that's a here's austria that k |
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0:01:52 | years austria later j |
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0:01:55 | so whenever one of those received signal emitted by oscillator |
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0:01:59 | i |
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0:02:00 | it will adjust |
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0:02:02 | it will adjust according to our update function |
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0:02:06 | this means basically that are not later that is in the lower ha |
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0:02:12 | will jump |
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0:02:13 | for words |
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0:02:14 | and then also later that is in the above |
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0:02:17 | will jump backwards |
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0:02:20 | that the main idea of the update function is to oscillators |
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0:02:24 | one the d m at their |
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0:02:27 | of the set |
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0:02:28 | the i |
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0:02:30 | and we will not know that is the i |
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0:02:33 | we monotonically decreases |
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0:02:35 | for combination of how this applies to bigger is that of oscillators |
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0:02:39 | will not be shown in the video |
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0:02:42 | on the left we see realization with ten oscillators on the random network |
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0:02:47 | if i of an oscillator is indicated by red light |
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0:02:51 | on the top right we show the oscillator spaces at the five times |
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0:02:55 | note that the y-axis is centered around zero |
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0:03:01 | well oscillators between the plot lines are combined in a set s |
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0:03:05 | on the bottom right with you did em at their of this and the size |
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0:03:09 | of face |
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0:03:10 | as soon as well oscillators are you know s then d s equals d i |
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0:03:15 | and is monotonically decreasing and synchronization is achieved |
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0:03:23 | after all this technical detail |
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0:03:27 | we are now able to see the bigger picture |
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0:03:30 | we guaranteed synchronisation |
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0:03:32 | for arbitrary network conditions |
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0:03:35 | for arbitrary individual the late |
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0:03:38 | and sarcastic interactions |
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0:03:42 | did not give the guarantee |
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0:03:44 | and that and out that to better include those things for applications |
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0:03:49 | such as they may connect works |
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0:03:51 | robert swarming |
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0:03:54 | and network protocols for wireless communications |
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0:03:59 | thank you |
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