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