As important analysis tools, microscopes with high spatial resolution are indispensable for scientific research and clinical diagnosis. We report a proof-of-principle experimental demonstration of a two-arm microscope scheme and show that, by measuring the second-order correlation of light fields, more details of an object can be obtained through recording more information about the initial illumination field. The effects arising from the transverse coherence length and the axial correlation depth of the illumination field are also discussed.

An optically addressed liquid crystal modulator for wavefront control of 1053 nm laser beam is reported in this paper. Its working principle, control method and spatial phase modulation capability are mainly introduced. A new method of measuring the relationship between gray level and phase retardation is proposed. The rationality of the curve is further confirmed by designing special experiments. According to the curve, several spatial phase distributions have been realized by this home-made device. The results show that, not only the maximum phase retardation is larger than $2\unicode[STIX]{x03C0}$ for 1053 nm wavelength, but also the control accuracy is high. Compared with the liquid crystal on silicon type spatial light modulator, this kind of modulator has the advantages of generating smooth phase distribution and avoiding the black-matrix effect.

High laser damage threshold optical switches and spatial light modulators are in urgent demand in high power laser fields. In this Letter, liquid crystal optical switches using Si-doped GaN and Mg-doped GaN as transparent electrodes are fabricated, and the influence of the conductive properties of GaN is analyzed. The transmission and absorption characteristics of GaN and its sapphire substrate are tested. The results show that the liquid crystal device based on gallium nitride can be expected to play an important role in the fields of visible and near-infrared laser regions with a high laser damage threshold of more than 1 J / c m 2 .