The quantum-statistical characteristics of the field at the output port of an interferometer with a phase-conjugate mirror are evaluated. The explicit form of the density matrix of the field at the output port is given. The effect of an attenuator in the other arm of the interferometer is also discussed.
A quantum-statistical description of noise in interferometers is given in terms of the Wigner distribution function. The interferometer may contain an amplifier in one of its arms. The input field can be in a variety of states such as a Fock state, a coherent state or a squeezed coherent state. The Wigner function of the output field at the detector is shown to have a general Gaussian form with non-zero complex field amplitude and with other parameters related to the characteristics of the input field, amplifier and beam splitters, etc. An explicit form of the photon-number distribution is given. Higher-order correlations of the output field can be obtained from the Gaussian property of the Wigner function.
We study theoretically a Fabry–Perot interferometer with one phase-conjugate mirror. Comparisons with results previously obtained by Kastler [ Appl. Opt.1, 17 ( 1962)] for an ordinary Fabry–Perot interferometer are made. Specifically, we discuss the field intensity of the light both outside and inside the interferometer. We also study the intensity of the exterior field that is due to atoms radiating incoherently inside the interferometer. The operating characteristics below the threshold of the interferometer when it is filled with a gain medium are also analyzed and are found to be different from those of the ordinary interferometer. Finally, conditions are obtained under which the cavity can act as a regenerative amplifier.