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paraxial approximation
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z Eq Hj r I DL y j x
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far field
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E = ? E = ?
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x y z ’ x’, y’ paraxial approximation
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x y z ’ x’, y’ 2d version of the Fourier integral
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a b x y z ’ x’, y’ uniform illumination
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a = p/2 b = p/2
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a = p b = p/2
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a = p b = p
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a = 3p b = 3p
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x y z ’ x’, y’ 2zo
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The field @ z = +z0 is the Fourier transform of the field @ z = -z0
There is loss at the edges but this is very small Goubau – Schwering beam waveguide
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Normal propagation for a distance 2zo S’ losses
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University of Wisconsin
Elmer Scheibe James Beyer James Mink
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