Lecture 2 Flashcards
angular resolution (formula)
α = 1.22 λ/D
resolution improves with
scale
Fraunhofer diffraction
plane-parallel waves incident upon aperture
viewed in far field L»_space; D^2/λ
2D Fourier transform of aperture
Up ∝ ∫ ( ∫ A )A(x,y) exp(-i(xkx+yky)dxdy
A single-slit is modelled mathematically as
a step function
A(x) = { 1 , -a < x < a
{ 0 , elsewhere
Intensity in a single slit is proportional to
|Up|^2
the modulus of the fourier aperture function squared
Bessel functions
Up = Uo [ 2J1(kα) / kα ]
first zeros for kα = 1.22 π
Geometrical optics
Image formed of object at point of convergence rays.
Consider object to be made up of many individual point sources.
One-to-one mapping
Spacing in the image plane governed by the magnification of the system
Image formation
When imaging an object at infinity, the image plane is simply the focal plane
Mapping between incident angle and position on focal plane
Point Spread Function (formula)
I(α) = Ig * I(PSF)
I(α) = image intensity
Ig = geometrical image intensity
I(PSF) = point spread function intensity
Point spread function (formula in words)
actual image is the convolution of the ideal image predicted by geometrical optics with the point spread function intensity
U(PSF) =
Uo [ 2J1(πDα/λ) / (πDα/λ) ]
I(PSF) =
Io [ 2J1(πDα/λ) / (πDα/λ) ]^2
diffraction limit
effects of aberrations are negligible, said to be diffraction limited
Resolution - Strehl Ratio (formula)
S = I(PSF)(0) / I(airy)(0)