| 0:00:03 | welcome to the video clip introducing or on the proportion of the new macroscopic quantum |
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| 0:00:09 | system |
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| 0:00:10 | my name is then as time from the institute of quantum physics or anyone university |
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| 0:00:17 | the question how can you want in the face |
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| 0:00:20 | and we also and controlled at a macroscopic scale so big interest |
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| 0:00:25 | so the foundational quantum mechanics |
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| 0:00:28 | in our paper we show that it is possible to tune to fractional just as |
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| 0:00:33 | what is known just as injunction from the classic |
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| 0:00:37 | into the ontology |
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| 0:00:40 | and obtain in this way a system in which you can also and control macroscopic |
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| 0:00:44 | on something on |
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| 0:00:47 | in the following two animations i will explain you the quantum effects which we also |
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| 0:00:53 | so |
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| 0:00:54 | and then all device works in principle |
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| 0:00:59 | in this in the picture or whatever the production |
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| 0:01:02 | according to can theoretically be i one |
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| 0:01:06 | or the other well |
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| 0:01:08 | but it quantum mechanical calculation shows |
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| 0:01:11 | that if the barrier becomes more enough |
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| 0:01:15 | the particle can times through the very |
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| 0:01:18 | this means |
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| 0:01:19 | when we start and one where of the potential and wait for some time |
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| 0:01:23 | it will appear in the second one |
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| 0:01:26 | when we meet again for the same time |
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| 0:01:28 | it will reappear in the first one |
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| 0:01:31 | in our paper we show that our system can be humans from a classical talk |
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| 0:01:38 | on television by lowering the barrier separating the two classical states |
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| 0:01:43 | but how does our system works |
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| 0:01:45 | all system consist of a long just as a function that is too long layers |
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| 0:01:50 | of syllable conduct of the corrected by an insulating battery |
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| 0:01:54 | we attach a pair of tiny current injectors to one of adjustable conducting on it |
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| 0:01:58 | shows |
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| 0:01:59 | here we inject current to one injector and collected from the other one |
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| 0:02:05 | this causes a strong gradient of the face of the simple conducting way function between |
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| 0:02:10 | the two injectors |
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| 0:02:11 | and in turn used to a strong gradients of the just isn't face |
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| 0:02:16 | which promotes new appearance of the and just isn't what |
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| 0:02:20 | this is the vortex of circulating around |
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| 0:02:23 | post magnetic flux can be controls |
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| 0:02:26 | by the injector occurrence |
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| 0:02:28 | another possible state for the same injected current it is complementary politics |
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| 0:02:34 | by applying now the same current twisting to help inject occurrence |
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| 0:02:38 | we may i say |
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| 0:02:40 | the same what is also the disposition |
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| 0:02:45 | strong states of a system which was this database consisting of two what is this |
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| 0:02:49 | with what was the durational circulating current |
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| 0:02:52 | post a test data |
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| 0:02:54 | and have the same energy |
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| 0:02:57 | in our paper we show that the dynamics of these two states can be mapped |
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| 0:03:00 | to the dynamics of a good know that would attention |
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| 0:03:04 | moreover we show that by decreasing the current |
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| 0:03:07 | the burial this effect of potential screen |
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| 0:03:10 | in our system can be you want from the classical into the pointing regime |
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| 0:03:15 | random oscillations are also available |
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| 0:03:18 | and we show that this situation can be established but temperatures below one hundred ninety |
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| 0:03:23 | two |
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| 0:03:24 | more parameters and it you can solutions of the what it's molecules |
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| 0:03:29 | and details for the tuning process a given you know paper |
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| 0:03:33 | and joy reading it |
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