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We demonstrate that two incoherently pumped atoms coupled to an optical resonator produce light with position-dependent field and intensity correlations. The fluorescence spectrum may comprise one, two or three peaks, while the second-order correlation function exhibits bunched or antibunched photon statistics depending on the position of the measurement. These dynamical quantum effects are connected to cavity-induced anticorrelation of the atomic dipoles (Phys. Rev. Lett., 79 (1997) 2650).

A scheme which results in the simultaneous narrowing of all three spectral peaks of the Mollow triplet is proposed. In particular, we investigate the effect on resonance fluorescence of processing the squeezed output of an optical parametric oscillator by propagation through a linear dielectric. The frequency-dependent squeezing phase induced by this process is found to result in subnatural spectral widths for appropriate parameter choices. The line-narrowing mechanisms at the Rabi sidebands manifest themselves in the second-order correlation function of the fluorescent field which is found to decay at a subnatural rate. The potential for experimental realization of these phenomena is discussed.

We present an analytical technique for investigating the behaviour of a coherently driven atom damped by a squeezed vacuum with finite squeezing bandwidth. A master equation and analytic expressions for the fluorescent spectrum are derived for the simple case of a two-level atom exactly resonant with the frequencies of both the squeezed field and the driving field. Suitable choices of driving strength, phase and squeezing source lead to either sub-natural lincwidths of the Rabi sidebands or a sub-natural linewidth of the central spectral peak or indeed sub-natural linewidths of all three spectral peaks when squeezing bandwidths are taken into account. We also establish the remarkable result that in the strong driving regime, the width of the central peak of the fluorescent spectrum depends solely on the squeezing found at the Rabi sideband frequencies.

Two-mode squeezed Gaussons are non-classical states of light which are intermediate between single-mode and two-mode squeezed states. They may be prepared by coherently mixing two single-mode squeezed states at a beam-splitter or via a frequency converter. When equally squeezed single-mode squeezed states are incident on a 50/50 beam-splitter the output will range between a two-mode squeezed state and two single-mode squeezed states as the phase of the input squeezed light is varied. This behaviour is reflected when the properties of such states are investigated.