Diffraction Flashcards

1
Q

What is diffraction?

A

The tendency of light (or any wave) to bend around objects

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2
Q

Why is it hard to see diffraction

A

Poor source temporal or spatial coherence masks the diffraction ripples

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3
Q

What is required to properly see diffraction

A

A point source
because any off axis rays will blur the shadow

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4
Q

When passing a wave through a slit, how does the slit size affect the diffraction pattern

A

as the size of the slit reduces towards the wavelength of the wave, the diffraction pattern will be more pronounced

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5
Q

Where does fresnel diffraction occur

A

in the near field, close to the slit

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6
Q

Where does Fraunhofer diffraction occur

A

In the far field, far from the slit

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7
Q

what is the distinction between interference and diffraction

A

interference involves the production of two or more separate beams
diffraction occurs naturally when a single wave is limited in some way

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8
Q

What is the Huygens-Fresnel Principle

A

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

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9
Q

What approach will be used to solve diffraction problems

A

Scalar Wave Approximation

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10
Q

What is the scalar wave approximation

A

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

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11
Q

What assumptions do we make about the aperture and the observation region for diffraction

A
  • 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
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12
Q

What is the problem with Kirchoff’s diffraction assumptions

A

they can be shown to yield zero field everywhere

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13
Q

What is the field in the observation plane for diffraction given by

A

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(…)=(1/iπœ†)(exp(ikr01)/r01)
r01 = sqrt(z^2 + (x0-x1)^2 + (y0-y1)^2)

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14
Q

Why can we not approximate r01 in the exp of h(…)=(1/iπœ†)(exp(ikr01)/r01)

A

it gets multiplied by k, which is big and so small changes in r01 can make a big difference

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15
Q

In Fresnel diffraction when do we approximate r01, abd what is the approximation

A

in the denominator it is approximated by z

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16
Q

What is the second approximation for Fresnel diffraction simplification

A

πœ€ β‰ͺ 1, sqrt(1 + πœ€) β‰ˆ 1 + πœ€/2 where πœ€ is the x’s and y’s

17
Q

What does the Fresnel integral yield

A

the light wave electric field at the distance z from the screen

18
Q

What is the fresnel integral

A

𝐸 (π‘₯1, 𝑦1) = exp (π‘–π‘˜π‘§)/(π‘–πœ†π‘§) exp [π‘–π‘˜ (π‘₯1^2 + 𝑦1^2/2𝑧] double integral over 𝐴(π‘₯0,𝑦0) exp {π‘–π‘˜ [(βˆ’2π‘₯0π‘₯1 βˆ’ 2𝑦0𝑦1)/(2𝑧) + (π‘₯0^2 + 𝑦1^2)/(2𝑧)]} 𝐸(π‘₯0, 𝑦0) 𝑑π‘₯0𝑑𝑦0

19
Q

What do we typically assume about the wave incident on the aperture for diffraction

A

It is a plane wave with exp(i(wt-kz)) constant wrt x0 and y0

20
Q

What is the final fresnel integral if we ignore the factors in front and explicitly write the aperture function

A

𝐸 (π‘₯1, 𝑦1) ∝ double integral over -∞ to ∞ exp {π‘–π‘˜ [(βˆ’2π‘₯0π‘₯1 βˆ’ 2𝑦0𝑦1)/(2𝑧) + (π‘₯0^2 + 𝑦1^2)/(2𝑧)]} A(π‘₯0, 𝑦0) 𝑑π‘₯0𝑑𝑦0

21
Q

What does Fresnel theory predict for the pattern if a wave encounters a stop

A

it develops a hole (shadow of circular obstacle) which fills from the centre first as the beam diffracts, at quite a high irradiance with a bright spot - called poisson’s spot

22
Q

What if the diffraction from an array of slits

A

the talbot effect says an array of slits produces a beam pattern which alternates between 2 fringe patterns