Diffraction Flashcards
What is diffraction?
The tendency of light (or any wave) to bend around objects
Why is it hard to see diffraction
Poor source temporal or spatial coherence masks the diffraction ripples
What is required to properly see diffraction
A point source
because any off axis rays will blur the shadow
When passing a wave through a slit, how does the slit size affect the diffraction pattern
as the size of the slit reduces towards the wavelength of the wave, the diffraction pattern will be more pronounced
Where does fresnel diffraction occur
in the near field, close to the slit
Where does Fraunhofer diffraction occur
In the far field, far from the slit
what is the distinction between interference and diffraction
interference involves the production of two or more separate beams
diffraction occurs naturally when a single wave is limited in some way
What is the Huygens-Fresnel Principle
every unobstructed point in a wavefront at a given instant serves as a source of spherical secondary waves.
amplitude of the optical field at any point beyond is the superposition of all these wavelets
What approach will be used to solve diffraction problems
Scalar Wave Approximation
What is the scalar wave approximation
discard the fact that light consists of two oscillating vector fields and imagine the wave in terms of a single scalar variable with angular frequency w and wave vector k
What assumptions do we make about the aperture and the observation region for diffraction
- assume the aperture region is much smaller than the observation region
- inside the aperture, the field and its spatial derivative are the same as if the screen were not present
- outside the aperture (in the shadow of the screen), the field and its spatial derivative are zero
What is the problem with Kirchoffβs diffraction assumptions
they can be shown to yield zero field everywhere
What is the field in the observation plane for diffraction given by
E(x1,y1) at a distance z from the aperture plane is given by a convolution
E(x1,y1) = double integral over A(x0,y0) = h(x1-x0,y1-y0)E(x0,y0)dx0dy0
h(β¦)=(1/iπ)(exp(ikr01)/r01)
r01 = sqrt(z^2 + (x0-x1)^2 + (y0-y1)^2)
Why can we not approximate r01 in the exp of h(β¦)=(1/iπ)(exp(ikr01)/r01)
it gets multiplied by k, which is big and so small changes in r01 can make a big difference
In Fresnel diffraction when do we approximate r01, abd what is the approximation
in the denominator it is approximated by z