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Spontaneous emission Standing waves

Figure Cl.4.5. Population modulation as the atom moves through the standing wave in the Tin-periD-lin one dimensional optical molasses. The population lags the light shift such that kinetic is converted to potential energy then dissipated into the empty modes of the radiation field by spontaneous emission (after 1171). Figure Cl.4.5. Population modulation as the atom moves through the standing wave in the Tin-periD-lin one dimensional optical molasses. The population lags the light shift such that kinetic is converted to potential energy then dissipated into the empty modes of the radiation field by spontaneous emission (after 1171).
Hence the only relevant modification of the spontaneous emission rate due to the presence of fhe parabolic mirror is fhe replacement of the plane traveling waves/(n,r) = by the standing waves... [Pg.478]

See other pages where Spontaneous emission Standing waves is mentioned: [Pg.326]    [Pg.744]    [Pg.470]    [Pg.857]    [Pg.152]    [Pg.251]    [Pg.1005]    [Pg.1178]    [Pg.127]    [Pg.381]    [Pg.275]    [Pg.125]   
See also in sourсe #XX -- [ Pg.226 , Pg.227 , Pg.228 , Pg.229 , Pg.230 , Pg.242 , Pg.243 , Pg.244 , Pg.245 , Pg.246 , Pg.247 , Pg.248 , Pg.249 , Pg.250 , Pg.251 ]



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