The wavelength of the light in the mica is l/m
= 322 nm, so the mica is 5l/4 thick and it introduces
a phase shift of p/2 to the light that passes
through it. This means that that portion of the Fourier transform
is multiplied by i. Let us assume that the slit extends from
–a/2
to a/2 in the x and y directions. The mica covers
the region x < 0. Thus the transmission function becomes

Since the x and y coordinates separate, we can calculate F(u) and multiply it by
.
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To convert from u to the diffraction
angle q, recall that
so that
A graph of this function (along the horizontal axis) is shown here,
together with the function for a slit with no mica.