Abstract
The recent realizations of squeezed states and phase-noise quenching via correlated spontaneous emission have sharpened the question of the relationship of quantum noise inside and outside a transmitting cavity. Although many authors1 have succeeded in demonstrating that the degree of quantum noise reduction in the transmitted field can be quite different from (and even much larger than) that in the intracavity field, a rigorous yet simple physical picture of the reasons for this curious fact has not emerged.
© 1990 Optical Society of America
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