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Passive crystal
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  • Passive crystal

Passive crystal

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Passive crystal

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Product Details

The center is thicker than the edge and has a converging effect on the light, so it is also called a converging lens. According to different shapes, convex lenses can be divided into biconvex lenses, plano-convex lenses and meniscus lenses, etc., by refracting light to change its propagation direction, so as to achieve the effect of image magnification, reduction, handstand or upright. The special shape leads to its unique optical properties. When the light passes through the cylindrical mirror, the light will be focused into a straight line or other forms of deformation. This property gives cylindrical lenses significant advantages in changing the size of the image, such as converting a point spot into a line spot, or changing the height of the image without changing the image width.

  • Product Description

    Physical Properties

     

    Chemical Molecules Cr 4+ :Y 3 A 15 O 12
    Crystal Structure Cubic Garnet
    Reduction Time 8.5μs
    Mohs Hardness 8.5
    Density 4.56g/cm3
    Crystal Orientation [100]+/-10°
    Thermal Conductivity 12.13W/m/K
    Refractive Index 1.82 @ 1064nm

     

    Optical Properties

     

    Ground State Absorption Cross Section δs1=4.3*10-18cm²
    Absorption Cross Section in Divergent State δs1=4.3*10-18cm²
    Fluorescence Lifetime 3.4us

     

    Capability

     

    Cr 4+ Doping Concentration 0.5 mol%~3 mol%
    Aperture 2x2~14x14mm
    Initial Transmittance 10% ~ 99%

     

    Physical Properties

     

    Dimensional Tolerance (W±0.1mm) X (H±0.1mm) x (L + 0.2mm/-0.1mm)
    Surface Shape <λ/8 @ 633nm
    Surface Finish Better than 10/5 Scracth/Dig per MIL-0-13830A
    Parallelism < 20 arc seconds
    Perpendicularity <5 arc minutes
    Transmitted Wavefront Less than λ/8 @ 633nm
    Clear Aperture > 90% Central Area
    Coating Anti-reflective

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