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Cavity fields photon statistics

To evaluate the mean number of photons and the statistical properties of the quantum field created in the cavity at t > T, we introduce the Hermitian quadrature component operators... [Pg.337]

The one-atom maser can be used to investigate the statistical properties of non-classical light [1298, 1299]. If the cavity resonator is cooled down to T < 0.5 K, the number of thermal photons becomes very small and can be neglected. The number of photons induced by the atomic fluorescence can be measured via the fluctuations in the number of atoms leaving the cavity in the lower level n — 1). It turns out that the statistical distribution does not follow Poisson statistics, as in the output of a laser with many photons per mode, but shows a sub-Poisson distribution with photon number fluctuations 70 % below the vacuum-state limit [1300]. In cavities with low losses, pure photon number states of the radiation field (Fock states) can be observed (Fig. 9.77) [1301], with photon lifetimes as high as 0.2 s At very low... [Pg.556]


See other pages where Cavity fields photon statistics is mentioned: [Pg.540]    [Pg.67]    [Pg.408]    [Pg.102]    [Pg.206]    [Pg.1296]    [Pg.121]    [Pg.325]    [Pg.206]    [Pg.23]   
See also in sourсe #XX -- [ Pg.337 , Pg.338 , Pg.339 , Pg.340 , Pg.341 , Pg.342 , Pg.343 , Pg.344 , Pg.345 , Pg.346 , Pg.347 , Pg.348 , Pg.349 , Pg.350 , Pg.351 , Pg.352 , Pg.353 ]




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