Abstract: Prior art coherent optical wave mixing has permitted two-dimensional maps from which coupled quantum transitions have been identified in molecular samples. However, extended signal accumulation times and computer processing are required for a detailed molecular analysis, which can lead to sample toxicity and difficulties in interpretation. These and other requirements are reduced by an apparatus arranged for the projection of an image that directly encodes quantum couplings from a sample. Such an apparatus includes a source component 36, a diffractive optical component 25 for generating at least three light fields 1, 2, 3 from one light field 23, one or more optical telescopes 26 and 27 wherein the transverse separation between optical paths is modified from that possible to define with a single telescope between common object and image points, a sample 11 containing said image point, and a means for resolving and detecting the angular variation of light emission from a sample.

Abstract: Prior art coherent optical wave mixing has permitted two-dimensional maps from which coupled quantum transitions have been identified in molecular samples. However, extended signal accumulation times and computer processing are required for a detailed molecular analysis, which can lead to sample toxicity and difficulties in interpretation. These and other requirements are reduced by an apparatus arranged for the projection of an image that directly encodes quantum couplings from a sample. Such an apparatus includes a source component (36), a diffractive optical component (25) for generating at least three light fields (1, 2, 3) from one light field (23), one or more optical telescopes (26) and (27) wherein the transverse separation between optical paths is modified from that possible to define with a single telescope between common object and image points, a sample (11) containing said image point, and a means for resolving and detecting the angular variation of light emission from a sample.

Abstract: In a solid state, optically end-pumped laser, the laser gain medium has a tapered diameter to minimize the maximum path length of barrelling amplified stimulated emission (ASE), and a roughened surface region at one end to scatter barrelling ASE out of the gain medium; thereby minimizing the negative effective of barrelling ASE's, and inhibiting the trapping of rays with a large longitudinal component, but disallowing a cyclic, i.e. repeated, pass path with specular reflections.