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Contrast properties of reflective liquid crystal light valves in projection displays

机译:投影显示器中反射型液晶光阀的对比度特性

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Projectors that use reflective light valves must employ beam splitters or analogous components to separate bright-state light from dark-state light, since both states must propagate in the space above the light valve. Polarization ray tracing shows that such beam splitters will not usually achieve high rejection of dark-state light when the beam has the typical angular divergence of about ±10°. At such propagation angles, different rays in the beam will have appreciably different planes of incidence at tilted optical coatings in the system (because of the compound angles involved). If the light valve is mirrorlike in dark state, we show that to correct the depolarization resulting from compound incidence angles, it is necessary that the optics introduce no rotation in the illuminating polarization. To a reasonable approximation, such a rotation in polarization will double in the return pass through the optics. To the same approximation, induced ellipticity in the illuminating polarization will cancel in double pass, and pure rotation can be converted to pure ellipticity with a quarterwave retarder. An important qualification, however, is that a light valve can only be exactly mirrorlike in restricted cases [i.e., if linearly polarized input light remains exactly linearly polarized (though possibly rotated) at all wavelengths when it reaches the mirror backplane of the light valve, independent of small manufacturing errors]. We calculate contrast loss in the more realistic case of a reflective twisted nematic liquid crystal (TNLC) light valve interacting with tilted coatings in the projection optics over finite numerical aperture (NA), and discuss the impact on LC thickness tolerances and spectral bandwidth Δλ. We extend our results to apply to more general light valves and more general projection optics configurations. Dark-state background is found to scale as NA2 (or in some cases as ∼NA2Δ&x03-n;BB;2). Because of this interaction, the complete system almost always shows a lower contrast than the light valve alone.
机译:使用反射光阀的投影仪必须使用分束器或类似组件,以将亮态光与暗态光分开,因为这两种状态都必须在光阀上方的空间中传播。偏振射线追踪表明,当光束的典型角发散度约为±10°时,此类分束器通常不会实现对暗态光的高抑制。在这样的传播角度,光束中的不同光线在系统中倾斜的光学涂层处将具有明显不同的入射平面(由于所涉及的复合角度)。如果光阀在黑暗状态下呈镜面状,则表明要校正由复合入射角引起的去偏振,必须使光学器件在照明偏振中不旋转。为了合理地近似,这种偏振旋转将使通过光学系统的返回光程增加一倍。近似地,照明偏振中的感应椭圆率将在两次通过中消除,并且可以使用四分之一波长延迟器将纯旋转转换为纯椭圆率。但是,一个重要的限定条件是,光阀只能在有限的情况下完全像镜子一样[即,如果线性偏振输入光到达光阀的镜子底板时,在所有波长下都保持线性偏振(尽管可能旋转),独立于小制造误差]。我们计算了在更实际的情况下,反射扭曲向列液晶(TNLC)光阀与投影光学系统中的倾斜涂层在有限数值孔径(NA)上相互作用时的对比度损失,并讨论了对LC厚度公差和光谱带宽Δλ的影响。我们将结果扩展到更通用的光阀和更通用的投影光学系统配置。发现暗态背景的缩放比例为NA2(或在某些情况下为〜NA2Δ&x03-n; BB; 2)。由于这种相互作用,整个系统几乎总是比单独的光阀显示出更低的对比度。

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    《IBM Journal of Research and Development》 |1998年第3期|P.359-386|共28页
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  • 入库时间 2022-08-18 01:47:37

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