0:00:05 | hello |
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0:00:06 | my name is you don't childish and this is de vito abstract what an article |
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0:00:11 | entitled along idea vertically the human electron you know wonder why we think or to |
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0:00:16 | be interaction |
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0:00:18 | publish in new journal of physics |
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0:00:21 | michael orders are professional drawn jeff's on and professor and blah natasha |
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0:00:28 | in this work we present an exact analytical solution for the weight function of an |
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0:00:33 | electron you know one dimensional semiconductor quantum via with thing or written direction |
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0:00:40 | which is driven by an external time dependent confining potential in which the position of |
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0:00:47 | the potential minimum style-independent in its shape is kept constant |
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0:00:53 | the eigen states of the and the remark only potential cameras that let's |
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0:00:59 | and the ground state grammars a tablet can be defined as it you |
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0:01:03 | due to the presence of this thing or reading direction the scene of an electron |
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0:01:08 | is rotated on the rocks you in the demon system |
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0:01:12 | indeed basically means these behavior has already been studied in the literature where it was |
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0:01:19 | shown that the rotation angle is directly proportional to the distance the potential well moves |
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0:01:25 | using our analytical solution we can generalize this result and shown that you be manipulation |
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0:01:32 | can also be exactly performed in the non-ideal that you could or g with a |
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0:01:37 | mean once the rotation times for word that the inverse quantum dot level space |
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0:01:43 | the solution allows analytical expressions for various quantities to be derived |
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0:01:49 | for example screen and those you know rotations |
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0:01:53 | energy and occupation probabilities for excited they |
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0:01:58 | the for quantum mechanical solution incorporates the solution for the corresponding classical harmonic and you're |
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0:02:05 | and we you examples for a few deriving schemes |
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0:02:09 | the fastest only directional driving that generates the perfect displacement without residual posts relations is |
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0:02:17 | given by a stand and displacement of the dot followed by waiting time of one |
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0:02:22 | half of the constellation time t not followed by another start and displacement of the |
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0:02:28 | belt |
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0:02:29 | with the appropriate total displacement these can for example generate a perfect being you |
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0:02:37 | we also consider you know ten |
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0:02:40 | and thus seamless i don't driving |
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0:02:43 | except for specific diving profile that a residual was to relations after the dogs |
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0:02:50 | but the those in expectation values remain constant regardless of the chosen driving |
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0:02:58 | for all that the writings consider the perfect syllables being transformations |
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0:03:04 | which she the electrode in the grounds they mainly for after the transit of the |
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0:03:09 | dot |
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0:03:09 | we always be done and even in the non idea that decoder g |
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0:03:15 | however |
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0:03:16 | during the forced evolution the state of the electron depends strongly on the degree of |
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0:03:22 | the non linear but these for an initial state in the ground state many for |
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0:03:27 | the time evolved they is the coherence they with probability of occupation of and excited |
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0:03:34 | forced to the interstate given by a possible this new after the low starts these |
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0:03:40 | probabilities think determined by the residual was relations |
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0:03:47 | in the article we present the exact solutions for an electron you know the demon |
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0:03:52 | quantum dot you know one dimensional quantum why we think or to be interaction the |
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0:03:58 | essence of formalism lives in the solution of a corresponding classical harmonic and you |
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0:04:04 | together with the education of no problem canonical transformation |
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0:04:11 | thank you for watching |
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