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  1. N. C. Gallagher, J. A. Bucklew, Appl. Opt. 19, 4266 (1980).
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Fig. 1
Fig. 1

Reconstructed image of a nondetour phase amplitude hologram using 12 subcells per sample cell.

Equations (9)

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h ( x , y ) = T 2 L sinc ( xT L ) m n k = 0 L 1 H mnk sinc ( H mnk xT ) exp { j 2 π T [ ( n + k L ) x + my ] } ,
h ( x , y ) = m n F 1 [ A ( u , υ ) L k = 0 L 1 cos [ θ ( u , υ ) 2 π k L ] μ { cos [ θ ( u , υ ) 2 π k L ] } exp ( j 2 π kn L ) ] * δ ( x n / T , y m / T ) ,
cos ( x ) = ½ [ exp ( jx ) + exp ( jx ) ] μ [ cos ( x ) ] = 1 2 + 2 π r = 0 ( 1 ) r ( 2 r + 1 ) cos [ ( 2 r + 1 ) x ] = 1 2 + 1 π r = 0 ( 1 ) r ( 2 r + 1 ) { exp [ j ( 2 r + 1 ) x ] + exp [ j ( 2 r + 1 ) x ] } .
h ( x , y ) = m n F 1 ( A ( u , υ ) 4 L { exp ( j θ ) k = 0 L 1 exp [ j 2 π k L ( n 1 ) ] + exp ( j θ ) k = 0 L 1 exp [ j 2 π k L ( n + 1 ) ] } ) * δ ( x n / T , y m / T ) + other terms .
h ( x , y ) = m F 1 [ A ( u , υ ) 4 exp ( j θ ) ] * δ ( x 1 / T , y m / T ) = 1 4 m g ( x 1 / T , y m / T ) .
H mnk = A [ ( n + k L ) T , mT ] μ ( cos { θ [ ( n + k L ) T , mT ] 2 π k L } ) .
h ( x , y ) = m n F 1 [ A ( u , υ ) L k = 0 L 1 μ { cos [ θ ( u , υ ) 2 π k L ] } exp ( j 2 π kn L ) ] * δ ( x n / T , y m / T ) .
h ( x , y ) = m n F 1 ( A ( u , υ ) π L k = 0 L 1 r = 0 ( 1 ) r ( 2 r + 1 ) exp ( j 2 π n L ) exp { ( 2 r + 1 ) [ θ ( u , υ ) 2 π k L ] } ) * δ ( x n / T , y m / T ) + other terms .
h ( x , y ) = m F 1 [ A ( u , υ ) π exp ( j θ ) ] * δ ( x 1 / T , y m / T ) = 1 π m g ( x 1 / T , y m / T ) .

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