
126 ◾ Kieran G. Larkin
Assuming that the local fringe structure induced by phase changes
faster than the amplitude, then a small region of the fringe pattern can be
expanded as a Taylor series of the phase Ψ:
−=+ψ +ψ +ψ +−ψ+ψ+ψ(,)(,)
{exp[( )] exp[
]}
00 10 01
00 10 01 00 10 01
gxyaxy
b
ixyi
(4.11)
e forward and inverse Fourier transforms in 2-D are dened by
∫∫
== −π +
+∞
+∞
(,)F{(,)}(,)exp[ 2( )]Guvgxy gxyiux vy dxdy
(4.12a)
and
∫∫
== +π +
−
+∞
+∞
(,)F{(,)}(,)exp[ 2( )]
1
gxyGuv Guviux vy dudv (4.12b)
e (local) 2-D Fourier transform of these equations is simply two
Dirac delta side lobes:
=δ−− +ψ +δ ++ −ψ
{( ,)exp[ ]( ,)exp[ ...