| 0:00:07 | in the l two thousand and ten researchers use of their speaker quite a transition |
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| 0:00:13 | we can also mean both competing they inspired |
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| 0:00:16 | and optical cavity their to compensate this problem by stress oscillator |
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| 0:00:21 | the author that's a very critical value of the later intensity |
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| 0:00:26 | the content the catskills |
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| 0:00:28 | the later be into the cavity which causes only in the number of photons inside |
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| 0:00:34 | the cavity |
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| 0:00:35 | at the same time they and optical potential or inside the cavity for the outcomes |
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| 0:00:41 | of the compensate which result in the organisation of actual |
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| 0:00:46 | you get a transmission in then after the change of the momentum state of the |
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| 0:00:52 | actual |
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| 0:00:54 | in our work we generalize and by considering two more calls session content inside the |
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| 0:01:00 | one dimensional optical cavity here each optimal compensate has to hyper state which are called |
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| 0:01:07 | increment by their you can you to an extracted the state |
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| 0:01:12 | well the transition is extracted the highest operated because of a tuning easy to see |
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| 0:01:18 | from the transition frequency |
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| 0:01:21 | and the result of this roman helping there will be too |
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| 0:01:25 | effective potential in the dynamical equations we one and v two maybe one is the |
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| 0:01:31 | rate of formant transition which couples two different high blind date but we to the |
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| 0:01:37 | starting rotation or something hyper final state c |
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| 0:01:41 | what angel are modulated by capital bold and therefore roman transition had maximum rate on |
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| 0:01:49 | the on signals of the county mode and at the same time we can that |
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| 0:01:52 | attract potential to have meaning not exactly on the on signal |
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| 0:01:57 | it is not a problem a unique content they have all in the high and |
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| 0:02:03 | eight p |
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| 0:02:05 | david transmission comes from the final state be too high by the c and there |
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| 0:02:11 | are changing the maximization and on signal by the atoms and all remaining on top |
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| 0:02:19 | twenty five phase transition you know how simulation of in one of the dynamics of |
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| 0:02:24 | some importance quantities that all the number of what was inside the cavity and so |
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| 0:02:30 | in my recognition that we choose the normalized population difference of the two high one |
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| 0:02:36 | day |
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| 0:02:37 | i know that for the parameter domain shows the overlap polarization the cavity mode by |
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| 0:02:44 | and finally my position density |
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| 0:02:48 | you see the results of simulations then which is found by contrast there's later it |
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| 0:02:54 | and intensity are higher than the critical value which is need this formant transition |
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| 0:02:59 | and all the quantities indicate a sensation at the same time |
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| 0:03:04 | on the other eye fixation density as a function of time position shows formation of |
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| 0:03:10 | the magnetic not exactly at the time of formant transition maximization is changed on single |
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| 0:03:18 | of the cavity more do you sure and transition |
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| 0:03:22 | but increase the intensity of the we can have even if the magnitude that is |
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| 0:03:29 | so i know what the use of these magnetic lattices which are even after tuning |
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| 0:03:34 | the problem if all these lattices large number this means there'll at decide which are |
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| 0:03:40 | combined in a compact uncontrollable cavity quantum initial dynamics environments |
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| 0:03:45 | but how about exploring magnetic special property is in an is important entanglement |
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| 0:03:52 | random formation application |
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| 0:03:54 | or money to face transitions |
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| 0:03:58 | and you are watching |
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