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magnification of 1-3X and 2-8X corrects for laser beam divergence Edmund Optics (EO), the premier provider of optical ..... 2-8X with adjustable focus to correct for laser beam divergence . Ideal for high power laser applications Edmund Optics
optical communications, and imaging, their high beam divergence (typically about 48º for ridge-waveguide devices ..... minimized. The 200 mW tapered QC lasers have a horizontal beam divergence of only 6.6º in the single-lobe far field at
illumination for distances upto several hundred meters. VCSEL based illuminators are free from speckle and has a beam divergence of 18 deg. Custom configuration would be available for <1 deg divergence. The illuminator does not need any cooling
semiconductor lasers have a wide beam divergence , requiring bulky optics and ..... semiconductor lasers with an intrinsic beam divergence 25 times smaller than that of conventional ..... plasmonic collimator to narrow the beam divergence of quantum-cascade-laser
noise less than 0.5% from 10 H¥to 50 MHz. Power consumption is 10 W from a standard 110/220 Vac line. Beam divergence is 2 mrad, and beam diameter is less than 0.4 mm. The rms stability over two hours is 3%. The system, for applications
devices work at 1310 or 1550 nm and offer insertion loss of less than 0.3 dB and return loss of less than -60 dB. Beam divergence is less than 0.20°, and a typical collimated beam diameter is 430 µm. LightPath Technologies, Albuquerque
planetariums. The laser runs on 220-V, 50-A single-phase power or a 208-V, 30-A three-phase power supply. Beam divergence is less than 4 mrad, and beam diameter at exit aperture is 6 mm. The laser resonator measures 40 ¥ 8 ¥ 19 in
and planetariums. The laser runs on 220-V 50-A single-phase or a 208-V 30-A three-phase power supply. Beam divergence is less than 7 mrad, and beam diameter at exit aperture is 4 mm. The laser resonator measures 40 ¥ 8 ¥ 19 in
spectral width of 120 nm full width at half maximum (FWHM), a 250 mW average power, an 80 MHz repetition rate, and a beam divergence of about 0.1°. To start, the pulses were reflected along the prism axis of the retroreflector for no relative
a 4.8 m total computer-controlled optical delay. Before entering the delay line, a 2X telescope reduces the beam divergence . A block diagram shows how to create a delay for pump-probe experiments by synchronizing two amplifiers, slave