The 63976-45QC-OA is a complete QTH light source featuring the 63358 45 W QTH Lamp, with NIST traceable calibration over a 300-1700 nm wavelength range. NIST traceable calibration is a useful advantage for calibrating other lamps or complete spectroscopy systems. This light source comes with a Certi..
The 77300 Grating Assembly is designed for installation into the Oriel 77250 Hand Operated Monochromator. This 30 x 30 mm grating comes pre-aligned in its own frame, allowing it precisely fit inside the instrument. The frame has a tab that allows the grating to be inserted or replaced inside the m..
The 77305 Grating Assembly is designed for installation into the Oriel 77250 Hand Operated Monochromator. This 30 x 30 mm grating comes pre-aligned in its own frame, allowing it precisely fit inside the instrument. The frame has a tab that allows the grating to be inserted or replaced inside the m..
The 10RP52-1B Achromatic Quartz-MgF2 Half Wave Plate consists of two different birefringent crystals: crystalline quartz and magnesium fluoride (MgF2). Enclosed in a 1 inch (25.4 mm) housing. This 18 mm aperture zero-order half waveplate has λ/2 retardation over a 400 to 700 nm wavelength ran..
The 10RP52-2B Achromatic Quartz-MgF2 Half Wave Plate consists of two different birefringent crystals: crystalline quartz and magnesium fluoride (MgF2). Enclosed in a 1 inch (25.4 mm) housing. This 18 mm aperture zero-order waveplate has λ/2 retardation over a 700 to 1000 nm wavelength range. ..
The 10RP54-1B Achromatic Quartz-MgF2 Quarter Wave Plate consists of two different birefringent crystals: crystalline quartz and magnesium fluoride (MgF2). Enclosed in a 1 inch (25.4 mm) housing. This 18 mm clear aperture zero-order waveplate has λ/4 retardation over a 400 to 700 nm wavelength..
The 10RP54-2B Achromatic Quartz-MgF2 Quarter Wave Plate consists of two different birefringent crystals: crystalline quartz and magnesium fluoride (MgF2). Enclosed in a 1 inch (25.4 mm) housing. This 18 mm clear aperture zero-order waveplate has λ/4 retardation over a 700 to 1000 nm wavelengt..
The 2117-FC Adjustable Gain and Bandwidth Balanced Fiber-Optic Receiver is an FC connectorized, 900 to 1700 nm photoreceiver with higher-gain and lower-bandwidth than our popular Model 20X1 laboratory photoreceivers. Ideal for FM spectroscopy, absorption spectroscopy, or ellipsometry, this InGaAs ad..
The 2117-FC-M Adjustable Gain and Bandwidth Balanced Fiber-Optic Receiver is an FC connectorized, 900 to 1700 nm photoreceiver with higher-gain and lower-bandwidth than our popular Model 20X1 laboratory photoreceivers. Ideal for FM spectroscopy, absorption spectroscopy, or ellipsometry, this InGaAs ..
The 2117-FS Adjustable Gain and Bandwidth Balanced Optical Receiver is a free space, 900 to 1700 nm photoreceiver with higher-gain and lower-bandwidth than our popular Model 20X1 laboratory photoreceivers. Ideal for FM spectroscopy, absorption spectroscopy, or ellipsometry, this InGaAs adjustable ba..
The 2117-FS-M Adjustable Gain and Bandwidth Balanced Optical Receiver is a free space, 900 to 1700 nm photoreceiver with higher-gain and lower-bandwidth than our popular Model 20X1 laboratory photoreceivers. Ideal for FM spectroscopy, absorption spectroscopy, or ellipsometry, this InGaAs adjustable ..
The F-H10-IR-APC Collimator is designed specifically for single-mode and polarization maintaining (PM) fiber applications in the 1000 to 1700 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 communicat..