An apparatus and method for optically remapping projected pixels to maximize the utilization and to optimize the distribution of remapped projection pixels to achieve optimal visual performance (generally uniform resolution and luminance). A device interposed between a projector and an imaging surface for optically remapping projected pixel locations with minimal aberration. When this device is interposed between a projector and an imaging surface, it changes the terminal location of each focused pixel such that it maximally coincides with the imaging surface, which is often a surface of complex curvature and very different from the native focal surface of the projector. One implementation of the technology includes a device that uses multiple optical surfaces.

A system and method to improve astigmatism correction and collimation of a laser beam generated by a diode in a low-level laser therapy system, but without using a complex optical configuration. A first divergent lens is a cylindrical lens. The divergence of the first lens is applied in the direction in which the diode's beam has relatively small divergence. The first lens creates divergence in the beam in a first axis, which divergence approximates the divergence in the perpendicular second axis. This first axis divergence corrects the astigmatism in the optical system of the therapy apparatus. The therapy apparatus thus can emit a beam with an elliptical cross-section with an axes ratio of less than 2:1, despite a high axes ratio of the beam originated by the diode. A second lens of the system and method is a collimating lens with elliptical shape adapted to maximize emitted beam collimation.

Device for generating a linear intensity distribution in a working plane (20), comprising at least one laser light source (11), optics (14) which shape the light (12) emitted by the at least one laser light source (11) in a first direction (X) and/or in a second direction (Y), a beam transformation device (13) increasing the beam quality factor (M.sub.x.sup.2) with respect to the first direction (X) and decreasing the beam quality factor (M.sub.y.sup.2) with respect to the second direction (Y), as well as an objective (17) acting in the second direction (Y) and a focusing device (18) acting in the second direction (Y), which is arranged behind the objective (17), wherein the objective (17) and the focusing device (18) image into the working plane (20) a plane (19) behind the beam transformation device (13) in which the light (12) in the second direction (Y) has an intensity distribution with a super-Gaussian profile or with a profile similar to a super-Gaussian profile.

An optical detector system provides output to an optical tracking system to facilitate optical communications by tracking a beam of incoming light using a fast-steering mirror (FSM). The optical detector system comprises an array of optical photodetectors, such array comprising one or more quad cells. The incoming light passes through one or more optical elements to generate a specified beam shape, such as a bar or cross, on the array. The resulting output from the array is highly responsive to changes in position of the reshaped beam on the array. As a result, noise equivalent angle (NEA) of the optical detector system representing pointing error is substantially reduced. A reduction in NEA facilitates more precise alignment, allowing incoming light to be aligned to a smaller area. For example, the incoming light may be aligned to a single mode optical fiber connected to a receiver system.

Disclosed is a combined lenses-based apparatus for line laser uniformity generation. The apparatus includes a laser diode, and an aspheric focusing lens and combined lenses that are arranged behind the laser diode sequentially. The combined lenses include a cylindrical lens and a plano-convex cylindrical lens. The cylindrical lens and the plano-convex cylindrical lens are arranged on an optical path sequentially. One end surface of the aspheric focusing lens is an aspheric surface. Light emitted by the laser diode is focused by passing though the aspheric focusing lens, and the combined lenses are able to disperse a focused beam into uniform line laser.

A polarization control member includes a first dichroic mirror having a first incident face, a second dichroic mirror joined to the first dichroic mirror, the second dichroic mirror having a second incident face, and a waveplate joined to the first incident face of the first dichroic mirror.

A divergence reshaping apparatus for laser diodes having a fast axis and a slow axis includes a fast axis collimator element having positive optical power in the fast axis and no optical power in the slow axis. A slow axis magnifier element has no optical power in the fast axis and positive optical power in the slow axis. An objective element has positive optical power in the fast axis and no optical power in the slow axis. A slow axis collimator element has negative optical power in the fast axis and positive optical power in the slow axis. Every element is optically aligned down an optical axis, and wherein a beam traveling through every element is collimated, compressed and shifted in the fast axis and expanded and collimated in the slow axis.

The optical system includes an optical element having a curvature in a first direction alone; and first and second lens array surfaces. Each of the lens array surfaces is provided with plural toroidal lens surfaces arranged in a second direction orthogonal to the first direction, the plural lens surfaces have a curvature mainly in the second direction, any lens surface on one of the lens array surfaces corresponds to one of the toroidal lens surfaces on the other, the direction of a first straight line connecting the vertexes of two toroidal lens surfaces corresponding to each other is orthogonal to the second direction, and in a cross section containing the first straight line and a second straight line that is in the second direction, one of the two toroidal lens surfaces is configured so as to form an imaging surface of the other for the object point at infinity.

A light synthesizing device includes first and second light emitting devices, first and second polarization control members, and a synthesis member. Each of the first and second light emitting devices has at least one first semiconductor laser element and at least one second semiconductor laser element, and configured such that a polarization direction of exit light from the first semiconductor laser element is different from a polarization direction of exit light from the second semiconductor laser element. The first and second polarization control members are respectively configured to change the polarization directions of the exit lights from the first semiconductor laser element of the first light emitting device and the second semiconductor laser element of the second light emitting device. The synthesis member is configured to combine light exited from the first light emitting device and light exited from the second light emitting device.

The present disclosure relates to an apparatus for forming a line beam. The apparatus includes a laser source, a telescope unit, a beam-transforming unit, a Fourier unit, a long-axis optical unit, and a short-axis optical unit. The laser source is configured to generate input light. The telescope unit is configured to magnify the input light in an X-axis direction perpendicular to an optical axis, which is a progression direction of the input light. The beam-transforming unit is configured to divide light incident from the telescope unit into a plurality of sub-columns. The Fourier unit is configured to uniformly mix the plurality of sub-columns. The long-axis optical unit is configured to uniformly disperse light mixed by the Fourier unit in the X-axis direction. The short-axis optical unit is configured to focus light passing through the long-axis optical unit onto a reference plane, wherein the short-axis optical unit includes a concave reflective surface, and a curvature of the reflective surface is maintained constant in the X-axis direction.