
Fluorescence Microscopy with Structured Excitation Illumination 553
B 26.2 I F
S O T F
T
he process of image formation can be described in
Fourier space. us, the Fourier-transformed uo-
rescence molecule distribution is multiplied by the
Fourier-transformed PSF, which is denoted as optical trans-
fer function (OTF). Applying a Fourier back-transformation
leads to the resulting image in real space.
In Fourier transformation theory, it can be shown that
any periodic function f(x) = f(x + L) (L is the period length)
is decomposable of sine and cosine functions (the so-called
Fourier series