1. Chapter 10 Diffraction
March 20 Fraunhofer diffraction: the single slit
10.1 Preliminary considerations
Diffraction: The deviation of light from propagation in a straight line.
There is no essential physical distinction between interference and diffraction.
Huygens-Fresnel Principle: Every unobstructed point of a wave front serves as a source of spherical wavelets. The amplitude of the optical field at any point beyond is the superposition of all these wavelets, taking into account their amplitudes and phases.
Fraunhofer (far field) diffraction: Both the incoming and outgoing waves approach being planar. a2/lR<<1, where R is the smaller of the two distances from the source to the aperture and from the aperture to the observation point. a is the size of the aperture. The diffraction pattern does not change when moving the observation plane further away.
Fresnel (near field) diffraction: The light source or the plane of observation is close to the aperture. General case of diffraction. The diffraction pattern changes when the observation plane moves. S P a R1 R2

2. A is the source strength.
Mathematical criteria for Fraunhofer diffraction:
The phase for the rays meeting at the observation point is a linear function of the aperture variables. S y' P
y' sinq
Waves from a point source:
Harmonic spherical wave:
A is the source strength. y x
P (x,y)
dy' r
-D/2
D/2
Coherent line source:
eL is the source strength per unit length.
This equation changes a diffraction problem into an integration (interference) problem.

3. 10.2 Fraunhofer diffraction 10.2.1 The single slity x
P (x,y) y' r
-D/2
D/2 R q
The slit is along the z-axis and has a width of D.
In the amplitude, r is approximated by R.
In the phase, r is approximated by R-y' sinq, if D2/Rl <<1.
Fraunhofer diffraction condition.
The overall phase is the same as a point source at the center of the slit.
Integrate over z gives the same function.

4. Example 10.1 y P (x,y) r y' R q x b D/2 -D/2 I/I(0)= 0.047 0.016
(©WIU OptoLab)
Example 10.1

5. Phasor model of single slit Fraunhofer diffraction: rolling paper

6. Read: Ch10: 1-2
Homework: Ch10: 2,7,8,9
Due: March 31

7. March 22 Double slit and many slits
The double slit z x
P (x,z)
R-a sinq R q a b
The result is a rapidly varying double-slit interference pattern (cos2a) modulated by a slowly varying single-slit diffraction pattern (sin2b/b 2).

8. Question:
Which interference maximum coincides with the first diffraction minimum?
(©WIU OptoLab)
Single-slit diffraction
Two-slit interference
Envelope
Fringes
“Half-fringe” (split fringe) may occur there. Our author counts a half-fringe as 0.5 fringe.
half-fringe

9. 10.2.3 Diffraction by many slitsz x
P (x,z)
R-a sinq R q a b
R-2a sinq

10. Subsidiary maxima (totally N-2):
Principle maxima:
Minima (totally N-1):
Subsidiary maxima (totally N-2): a
Example 10.3

11. Phasor model of three-slit interference: rotating sticks

12. Read: Ch10: 2
Homework: Ch10: 14,15,17
Due: March 31

13. 10.2.4 The rectangular aperture
March 24 Rectangular aperture and circular aperture
The rectangular aperture
Coherent aperture:
dS=dydz
P(Y,Z) r R x y z Y Z X
Fraunhofer diffraction condition

14. Rectangular aperture:
dS=dydz
P(Y,Z) r R x y z Y Z a b

15. Y minimum:
Z minimum:

16. F
P(Y,Z) R x y z Y Z q f r a
The circular aperture
Importance in optical instrumentation: The image of a distant point source is not a point, but a diffraction pattern because of the limited size of the lenses.
Bessel functions:.

17. J0(u)
J1(u) u q1
3.83
0.018
Radius of Airy disk: D P f
Example 10.6

18. Read: Ch10: 2
Homework: Ch10: 25,28,40
Due: March 31

19. Two coherent point sources:
March 27 Resolution of imaging systems
Equivalence between the far field and the focal plane diffraction pattern
Two coherent point sources: q P
a sinq R a y q P'
a sinq a f y' L
This applies to any number of arbitrarily distributed point sources in space.
Far field and focal plane produce the same diffraction pattern, but with different sizes.
R is replaced by f in the focal plane pattern.
A lens pulls a far-field diffraction pattern to its focal plane, reduces the size to f/R.

20. 10.2.6 Resolution of imaging systems
Image size of a circular aperture:
Rayleigh’s criterion for bare resolution:
The center of one Airy disk falls on the first minimum of the other Airy disk.
We can actually do a little better. D P f
Image size of a far point source: D P f
Angular limit of resolution:
Overlap of two incoherent point sources: D P2 S1 S2 P1
far away f

21. Human cone photoreceptor cells
Angular limit of resolution:
Human cone photoreceptor cells
150mm
Our eyes:
About 1/3000 rad
Spot distance on the retina: 20 mm/3000=6.7mm
Space between human photoreceptor cells on the retina: 5-7mm.
Pixel size of a CCD camera: ~7.5 mm.
Pupil diameter
Focal length
Wavelength dependence: CD DVD
Example 10.7

22. Read: Ch10: 2
Homework: Ch10: 42,46,49
Due: April 7

23. March 29, 31 Gratings
Diffraction grating: An optical device with regularly spaced array of diffracting elements.
Transmission gratings and reflection gratings.
Grating equation: qi qm a qi qm a
m=0 1 2 -2 -1 qi qr q0 a g
specular
0th
Blazed grating: Enhancing the energy of a certain order of diffraction.
Blaze angle: g
Specular reflection:

24. Grating spectroscopy:
Angular width for a spectral line:
N-slit interference Dq l
Between two minima, (N-1)p/N to (N+1)p/N .
Angular width of a spectral line due to instrumental broadening. Inversely proportional to Na.
Angular dispersion:
dqm dl

25. Barely resolved two close wavelengths:
Limit of resolution:
Barely resolved two close wavelengths:
(Dq)separation Dl
(Dq)width
Resolving power:
The resolving power increases with increasing order number and with increasing number of illuminated slits.

26. Free spectral range: m =3 m =2 m =1 sinqm
fsr
l l+Dl
In higher order diffraction the spectrum is more spread in angle. This results in a higher resolving power but a narrower free spectral range.
Example 10.9

27. Read: Ch10: 1-2
Homework: Ch10: 55,56,59,66,68
Due: April 7

28. “Everything is a lost horse.”