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Apr 29, 2009 ... The Optical Transfer Function (OTF) and ..... Consider the optical system from lecture 19, slide 16, with a pupil mask consisting of two holes, ...
Today

• Temporal and spatial coherence • Spatially incoherent imaging – The incoherent PSF – The Optical Transfer Function (OTF) and

Modulation Transfer Function (MTF)

– MTF and contrast – comparison of spatially coherent and incoherent imaging

next two weeks • Applications of the MTF • Diffractive optics and holography

MIT 2.71/2.710 04/29/09 wk12-b- 1

Temporal coherence

Michelson interferometer

If paths 1 & 2 are matched, then the recombined waveforms at the detector are correlated so they produce interference fringes. However, as the difference d2−d1 increases, the degree of correlation decreases and so does the contrast in the interference pattern.

random illumination (not single color anymore) detector

1 0.8

waveform from path 2, time delay t2=const+2d2/c

0.6

0.2

1

0

0.8

−0.2

0.6

−0.4

0.4

−0.6

0.2

E(t) [a.u.]

E(t) [a.u.]

0.4

por of e al dep e mit ted nden fiel ce d

−0.8

2

4

6

8

0

interference no interference (fields add coherently) (fields add incoherently)

−0.2

10

t [µ sec]

−0.4 −0.6 −0.8 −1 0

2

4

6

8

10

t [µ sec]

1

d2

tem

−1 0

0.9 0.8 0.7

I(d2−d1) [a.u.]

point source 1

d1

0.8

E(t) [a.u.]

MIT 2.71/2.710 04/29/09 wk12-b- 2

0.5 0.4 0.3

0.6

0.2

0.4

waveform at mirror 1,

time delay t1=const+2d1/c

0.6

0.2

0.1

0 −0.2

0 0

−0.4 −0.6 −0.8 −1 0

2

4

6 t [µ sec]

8

10

2

4

d2−d1 [µm]

6

8

10

Spatial coherence

Young interferometer 10

If holes 1 & 2 are coincident, or very closely spaced, then the recombined waveforms at the detector are correlated so they produce interference fringes. However, as the difference x2−x1 increases, the degree of correlation decreases and so does the contrast in the interference pattern.

waveform from hole 2, location x2

4

x [µm]

6

8

waveform from hole 1, location x1

x2 matched paths (equal time delay from the two holes to the detector)

1 0.9 0.8 0.7

I(x2−x1) [a.u.]

−1 0

x1

interference recorded near the bisectrix (almost matched paths)

E(x) [a.u.]

random waveform

−0.8

−0.6

−0.4

−0.2

0

0.2

0.4

0.6

0.8

2

interference no interference (fields add coherently) (fields add incoherently)

0.6 0.5 0.4 0.3 0.2 0.1 0 0

MIT 2.71/2.710 04/29/09 wk12-b- 3

2

4

x2−x1 [µm]

6

8

10

Field intensity in the coherent and incoherent cases

Perfectly coherent Intensity

2m×Ι0

Perfectly incoherent 0