A source module suitable for an optical coherence tomography system. The source module comprises a source operable to emit a divergent, source output beam either of circular cross-section (e.g. as output by a vertical cavity surface emitting laser) or of elliptical cross-section (e.g. as output by an edge-emitting semiconductor laser or diode). Collimation optics are provided to convert the source output beam into a non-divergent, collimated beam of elliptical cross-section having a major axis and a minor axis. A cylindrical lens is arranged with its plano axis aligned with the major axis of the elliptical collimated beam and its power axis aligned with the minor axis of the elliptical collimated beam so as to form a line focus extending along the major axis of the elliptical collimated beam.

A microscope apparatus 10 includes a detection optical system 12 that captures light from a sample S and an illumination optical system 11 that radiates an illumination light onto the sample S. The illumination optical system 11 includes a cylindrical lens 5 that has a power in a first-axis direction and does not have a power in a second-axis direction that is perpendicular to the first-axis direction, a cylindrical lens 6 that has a power in the second-axis direction and does not have a power in the first-axis direction, and a scanner 4 that scans the illumination light in a width direction. The illumination optical system 11 is configured such that the first-axis direction is the width direction described above, and the cylindrical lenses 5 and 6 are arranged posterior to the scanner 4.

An optoelectronic apparatus includes an array of emitters configured to emit respective beams of optical radiation. Projection optics include first cylindrical lenses, which have respective, mutually-parallel first cylinder axes, and are aligned respectively with the emitters in the array so as to receive and project the respective beams, and a second cylindrical lens, which has a second cylinder axis perpendicular to the first cylinder axes and is positioned adjacent to the first cylindrical lenses so as to receive and project all of the beams from the first cylindrical lenses.

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.

An anamorphic three-element objective lens projects a plurality of beams of different wavelengths and different diameters into an elongated focal spot in a working-plane. In one transverse direction of the lens, the beams are tightly focused with equal beam-waist widths in the working-plane, defining a height of the focal spot. In another transverse direction, the different beams are focused progressively beyond the working-plane such that the beams have a common beam-width in the working-plane, thereby defining a width of the focal spot.

A tubular lighting device encloses a plurality of LEDs and delivers light with uniformity, resembling the light delivered by a single linear light source. The tubular lighting device comprises a housing, a lighting chassis mounted on the housing, at least one circuit board with a plurality of LEDs mounted on the lighting chassis, each LED having a length A and two adjacent LEDs being separated by a distance L, a thin film mounted on the base and above the plurality of LEDs, the thin film being separated from the plurality of LEDs by a distance H, and a lens mounted on the lighting chassis and above the thin film.

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.

An optical lighting device includes an optical element having a light incident surface and a light emitting surface, wherein at least one first anamorphic asphere is deployed on either of the light incident surface or the light emitting surface. A first light source being square deployed on one side of the optical element and opposite to the light incident surface. The light source projects into the light incident surface, refracts by the first anamorphic asphere, transmits out of the light emitting surface and forms a predetermined light distribution area with a cut-off line on the upper fringe. Therefore, the optical lighting device has the advantage of simplified structure and high lighting efficiency.

Apparatus and methods for coupling an optical beam from an optical source to a hi-tech system are described. A compact, low-cost beam-shaping and steering assembly may be located between the optical source and hi-tech system and provide automated adjustments to beam parameters such as beam position, beam rotation, and beam incident angles. The beam-shaping and steering assembly may be used to couple an elongated beam to a plurality of optical waveguides.

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.