The Optics of Grating Light Valve Displays IKT 1 Contents Crash course in diffraction theory How to measure the width of a hair with a laser pointer How to design a grating light valve (GLV) display Questions and answers (hopefully) IKT 2 Diffraction of Light Maxwell’s equations may be reduced to the scalar wave equation. U may be any component of vectors H and E IKT 3 Diffraction of light Example solutions of the wave equation are the plane wave and spherical wave: IKT 4 Diffraction of light Light bends or diffracts around edges, and shrinking the size of an aperture will increase diffraction. IKT 5 Diffraction of light Light bends or diffracts around edges, and shrinking the size of an aperture will increase diffraction. IKT 6 Diffraction of light Light bends or diffracts around edges, and shrinking the size of an aperture will increase diffraction. IKT 7 The Huygens-Fresnel principle says: ”The light disturbance at a point P arises from the superposition of secondary waves that proceed from a surface situated between this point and the light source.” Augustin-Jean Fresnel Christiaan Huygens IKT 8 Diffraction of Light A mathematical representation of the HuygensFresnel principle: Spherical wave IKT 9 Diffraction of Light Far away from the aperture, and for small diffraction angles we may use the Fraunhofer approximation. U ( β ) = C ∫ U ( x) exp(ikβ x)dx S x β S IKT 10 Diffraction of Light Far away from the aperture, and for small diffraction angles we may use the Fraunhofer approximation. U ( β ) = C ∫ U ( x) exp(ikβ x)dx S x β S Fourier transform! IKT 11 Diffraction of Light We may now calculate the diffraction from a slit: ⎡ ⎛ kβ a ⎞ ⎤ ⎛ kβa ⎞ sin ⎜ sin ⎜ ⎟ ⎟⎥ ⎢ 2 ⎠ 2 ⎠ ⎥ ,I = ⎢ ⎝ U= ⎝ ⎛ kβa ⎞ ⎢ ⎛ kβa ⎞ ⎥ ⎜ ⎟ ⎜ ⎟ ⎥ ⎢ ⎝ 2 ⎠ ⎣ ⎝ 2 ⎠ ⎦ 2π k= 2 λ a β Minima for: β =m IKT λ a 12 Babinet’s principle The diffracted field from an aperture is the same as from an obscuration of the same size and shape IKT 13 What is the diameter of a hair? IKT 14 Diffraction from a grating light valve d IKT 15 Diffraction from a grating light valve h d ⎛ kβ d ⎞ sin ⎜ ⎟ 4 ⎠ 1 U= ⎝ ⎛ kβ d ⎞ N ⎜ ⎟ ⎝ 4 ⎠ ∑ [exp(ikβnd ) + exp(ikβ (n + N n =1 1 2 )d ) exp(2ikh)] IKT 16 The grating equation mλ sin β ≈ β = d d Phase difference = an integer number of wavelengths IKT 17 Diffraction from a grating light valve h d 2 I U 4 2 = = 2 sin (kh) I0 U0 π IKT 18 Diffraction from a grating light valve IKT 19 Diffraction from a grating light valve Angle given by the grating equation IKT 20 Diffraction from a grating light valve IKT 21 Diffraction from a grating light valve IKT 22 How to design a GLV display device IKT 23 How to design a GLV display device: Design targets 1000 pixels, 2000 horizontal resolution 10000 lumen total = 10 lumen per pixel 96 Hz refresh rate => 4 microsecond pixel time IKT 24 How to design a GLV display device: Design constraints Minimum feature size (gaps between ribbons) 0.6 µm Minimum ribbon distance 3 µm gives maximum diffraction angle and maximum throughput Required yield -> Maximum chip size Available laser light source (Xenon lamp is not powerful enough) IKT 25 Two display principles IKT 26 IKT 27
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