Abstract: A fluorescence microscope illumination method and a fluorescence assembly utilizing pulsed xenon lamp, wherein the fluorescence assembly comprises a wheel disc component, a camera component, and a light source component. The wheel disc component comprises a wheel disc mounting plate, on which a plurality of triple-hole fluorescent filter boxes are provided through a central shaft and a mounting shaft; a through hole is provided on the wheel mounting plate, and the mounting shaft is driven to rotate at a fixed angle, so that the boxes can stay in turn just below the through hole; the second stepper motor drives the side wheel disc to rotate at a fixed angle, so that the light source filter holes can stay in turn just in front of the lens. The invention can provide a microsecond-level high-brightness light source, greatly improve the photographing rate without reducing the image quality.

Abstract: A single-mode optical device, including a first region, and a second region laterally disposed about the first region, and including an absorbing layer and an isolation layer between the absorbing layer and the first region, wherein the thickness of the isolation layer is selected to control optical loss from the first region to the absorbing layer in the second region and thereby to attenuate one or more high order lateral optical modes of the device. The one or more high order lateral optical modes are attenuated relative to the fundamental lateral mode to provide the device with a high kink power. The device can be a 980 nm ridge diode laser where the thickness of an oxide insulating layer around the ridge is selected to control optical losses into a gold contact layer and thereby attenuate the first order lateral mode, providing the laser with a kink power of at least about 250 mW.

Abstract: A method of disordering a quantum well heterostructure, including the step of irradiating the heterostructure with a particle beam, wherein the energy of the beam is such that the beam creates a substantially constant distribution of defects within the heterostructure. The irradiating particles can be ions or electrons, and the energy is preferably such that the irradiating particles pass through the heterostructure. Light ions such as hydrogen ions are preferred because they are readily available and produce substantially uniform distributions of point defects at relatively low energies. The method can be used to tune the wavelength range of an optoelectronic device including such a heterostructure, such as a photodetector.

Abstract: A method of disordering a quantum well heterostructure, including the step of irradiating the heterostructure with a particle beam, wherein the energy of the beam is such that the beam creates a substantially constant distribution of defects within the heterostructure. The irradiating particles can be ions or electrons, and the energy is preferably such that the irradiating particles pass through the heterostructure. Light ions such as hydrogen ions are preferred because they are readily available and produce substantially uniform distributions of point defects at relatively low energies. The method can be used to tune the wavelength range of an optoelectronic device including such a heterostructure, such as a photodetector.

Abstract: A single-mode optical device, including a first region, and a second region laterally disposed about the first region, and including an absorbing layer and an isolation layer between the absorbing layer and the first region, wherein the thickness of the isolation layer is selected to control optical loss from the first region to the absorbing layer in the second region and thereby to attenuate one or more high order lateral optical modes of the device. The one or more high order lateral optical modes are attenuated relative to the fundamental lateral mode to provide the device with a high kink power. The device can be a 980 nm ridge diode laser where the thickness of an oxide insulating layer around the ridge is selected to control optical losses into a gold contact layer and thereby attenuate the first order lateral mode, providing the laser with a kink power of at least about 250 mW.