Concave mirrors are used in light collection applications or as focusing mirrors in imaging systems. Newport's concave metallic-coated mirrors on Borofloat 33 substrates provide a good combination of performance and value. They operate over a very broad spectral range – including UV to visible and visible to near-IR – with no chromatic aberration. For ultrafast applications, see our Ultrafast Optics Guide for more information on our concave mirrors designed specifically for use with ultrashort pulses.

Polarizingbeam splitterCube

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Polarization Beam splitterfiber

Ice Cube – Wire Grid Polarizing Beam SplitterWire Grid Versalight™ Polarizing Beam SplitterLaser Line Beamsplitting PolarizerBroadband Beamsplitting Polarizer

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Polarization beam splitterprice

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Polarization Beam Splitterthorlabs

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Polarizingbeam splitterprinciple

Precision Linear PolarizerHigh Contrast Linear PolarizerUltra-High Contrast Linear PolarizerGlan-Thompson PolarizerUltra-Broadband PolarizerMWIR PolarizerDeep Ultraviolet PolarizerWire Grid Versalight™ PolarizerDichroic Circular PolarizerBeam Separator

Precision Achromatic RetarderPrecision Superachromatic RetarderPrecision RetarderDual-Wavelength RetarderWide Field RetarderPolymer Film RetarderLarge Aperture RetarderBi-Crystalline Achromatic Retarder

Concave mirrors are used in light collection applications or as focusing mirrors in imaging systems. Newport's concave metallic-coated mirrors on Borofloat 33 substrates provide a good combination of performance and value. They operate over a very broad spectral range – including UV to visible and visible to near-IR – with no chromatic aberration. For ultrafast applications, see our Ultrafast Optics Guide for more information on our concave mirrors designed specifically for use with ultrashort pulses.

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The ICE Cube™ is assembled by embedding our polarizing beam splitter plate between two AR coated glass prisms. These cubes are designed with Nanowire® grid structures centered on the hypotenuse of the ICE Cube™. The ICE Cube™ PBS separates natural light into two main orthogonal, linearly polarized components; the p-polarized light which is transmitted while the s-polarized light is reflected at a 90° angle. In principle, half of the incident light is reflected, and the other half is transmitted.