The F-H5-VIS-APC Collimator is designed specifically for single-mode and polarization maintaining (PM) fiber applications in the 350 to 600 nm range, which need to generate a clean Gaussian Beam at any distance. It is designed for long distance projection applications such as free space communicatio..
The 10BPF10-350 Bandpass Filter is a 1 inch (25.4 mm) diameter band pass filter with a center wavelength of 350 ± 2 nm and a Full Width Half Max of 11 ± 2 nm. See Curve 6, for transmission graph. Our Bandpass Filters pass a narrow spectral band of UV, visible, or NIR radiation and reject out-of-band..
The 20BPF10-350 Bandpass Filter is a 2 x 2 inch (50.8 x 50.8 mm) square bandpass filter with a center wavelength of 350 ± 2 nm and a Full Width Half Max of 11 ± 2 nm. See Curve 6, for transmission graph. Our Bandpass Filters pass a narrow spectral band of UV, visible, or NIR radiation and reject out..
The 76596 Fiber Bundle Collimating Probe collimates the highly divergent outputs of fiber bundles. This beam probe is used to collimate the output from our fiber bundles with NA between 0.2 and 0.27, a 180 to 2200 nm spectral range, and θ1/2 Divergence Range of 0.15° to 0.50°. The lens is mounted in..
The 10BV70EAG.1 Femtosecond Optimized Silver Mirror is a concave mirror with a radius of curvature of 700 mm. It is 25.4 mm in diameter, 6.35 mm thick, and broadband optimized for 540 - 1000 nm. This ultrafast mirror is designed for zero to 45 degrees angle of incidence for S and P polarization. The..
The HPX350-60 HPFTM Fluorescence Bandpass Filter is 25.0 mm diameter, 4.3 mm thick band pass filter with nominal center wavelength at 350 nm and nominal bandwidth of 60 nm. It is manufactured to provide maximum performance delivering exceptionally high passband transmission (≥ 90%) and enhanced e..
The GB350 Granite Base Plate provides surface flatness to within 2 µm and features 3 point mounting to compensate for non-flat optical tables. Edge handles facilitate handling and locating the base plate on the work surface. They can be used to mount Ultra-Precision XM Series Linear Motor Stag..
The F-LA22 Laser Diode Aspheric Objective Lens has been specially designed for collimating and focusing laser diodes as well as fiber coupling. This version has a 0.25 Numerical Aperture (NA) and a 11.0 mm focal length with 5.5 mm clear aperture lenses. These lenses have all been corrected for the s..
The 6286 Mercury Arc Lamp contains an exactly measured amount of mercury and either argon gas or xenon which acts as a starter gas as the mercury vaporizes. This 1000 watt Hg lamp has a 0.8 x 2.7 mm effective arc size. When the lamp is cold, the gas pressure inside is lower than atmospheric and you ..
The KGA430-A Geltech Molded Glass Aspheric Lens is a very economic choice for collimating or focusing light at high magnification. It is made from Corning C0550 glass, which features low dispersion (Vd=50.40). Typical applications include fiber coupling, laser diodes, medical lasers, optical data st..
The KGA150-A Geltech Molded Glass Aspheric Lens is a very economic choice for collimating or focusing light at high magnification. It is made from Corning C0550 glass, which features low dispersion (Vd=50.40). Typical applications include fiber coupling, laser diodes, medical lasers, optical data st..
The KGA160-A Geltech Molded Glass Aspheric Lens is a very economic choice for collimating or focusing light at high magnification. It is made from Corning C0550 glass, which features low dispersion (Vd=50.40). Typical applications include fiber coupling, laser diodes, medical lasers, optical data st..