Fraunhofer Diffraction Flashcards

1
Q

Why does Fraunhofer diffraction use lenses

A

so that the source and fringe pattern can both be at convinient distances from the aperture

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2
Q

What are the requirements for fraunhofer diffraction to be observed

A

the incoming and outgoing waves approach being planar over the diffracting apertures or obstacles

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3
Q

What is crucial for determining the resultant field for Fraunhofer diffraction

A

the phase of each contribution at the screen due to differences in path traversed

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4
Q

how can path difference be described for planar wavefronts passing through an aperture

A

linear function of the 2 aperture variables

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5
Q

what is the definitive mathematical criterion for fraunhofer diffraction

A

linearity in the aperture variables

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6
Q

what is the formula for the aperture size

A

D^2 = x0^2+y0^2

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7
Q

what is the formula for fraunhofer diffraction if we neglect the phase factors and explicitly write the aperture function

A

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

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8
Q

What is notable about the fraunhofer diffraction formula

A

it is a fourier transform of the aperture field from one position x0 to another x1

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9
Q

How do you write the Fraunhofer diffraction in terms of the off-axis k vectors which are kx=kx1/z and ky=ky1/z

A

𝐸 (π‘˜π‘₯, π‘˜π‘¦) ∝ double integral from βˆ’βˆž to ∞ exp{βˆ’π‘– π‘˜π‘₯π‘₯ + π‘˜π‘¦π‘¦} 𝐴(π‘₯, 𝑦) 𝐸(π‘₯, 𝑦)𝑑π‘₯𝑑𝑦

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10
Q

How can we treat an aperture (single slit) of width b

A

divide it into N coherent point sources each of extent Ξ΄y=b/N

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11
Q

What can we say about point sources along an aperture which is uniformly illuminated by a plane wave

A

the amplitude of each point source is proportional to Ξ΄y, they are a source of spherical waves which would all be in phase

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12
Q

How do you evaluate the intensity of received wave at a point on a screen

A

the sum of all the waves arriving from all point sources in the aperture

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13
Q

In a direction ΞΈ, the wave emitted from a point source at y is out of phase with the wave emitted from y=0 by how much

A

kysinΞΈ

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14
Q

What is the field of a wave emitted from a point source at y on an aperture

A

𝛿𝐸 = 𝛿𝑦 exp(βˆ’π‘–π‘˜π‘¦π‘ π‘–π‘›πœƒ)

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15
Q

What is the intensity I(πœƒ) on the screen for a single slit aperture of width b

A

𝐼 (πœƒ) = 𝐼0 [sin 𝛽/𝛽]^2 = 𝐼0 sinc^2𝛽

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16
Q

what is the formula for sinc𝛽

A

sin𝛽/𝛽

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17
Q

What is the formula for 𝛽 where the wave approaches the slit at an angle i

A

𝛽=1/2 kb sinπœƒ = πœ‹/πœ† 𝑏 (sin i + sin πœƒ)

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18
Q

(in words) what is 𝛽

A

half the phase shift at angle theta across the aperture b

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19
Q

In single slit diffraction what is happening at the first zero?

A

the ray from the centre of the slit exactly cancels the edge ray due to the Ξ»/2 path difference and so on across the half slit

20
Q

What are the conditions for minima from single slit diffraction

A

I(πœƒ) = 0 when sin𝛽=0
𝛽 = +-mpi
sinπœƒ = mΞ»/b

21
Q

what are the conditions for maxima from single slit diffraction

A

𝛽=0 or when we minimise sinc^2𝛽
sin𝛽=0 or tan𝛽=𝛽

22
Q

Describe the fourier approach to fraunhofer diffraction from a slit

A

it is the fourier transform of a rect function which is the sinc function, hence the irradiance is sinc^2

23
Q

what is the fourier transform pair of a delta function

A

1

24
Q

what is the fourier transform pair of exp(iw0t)

A

2pi delta(w-w0)

25
Q

what is the fourier transform pair of cos(w0t)

A

pi [delta(w-w0)+delta(w-w0)]

26
Q

what is the fourier transform pair of sin(w0t)

A

pi/i[-delta(w-w0)+delta(w-w0)]

27
Q

what is the fourier transform pair of rect(t/T) top hat

A

Tsinc(Tw/2)

28
Q

what is the fourier transform pair of exp(-t^2/2T^2) gaussian

A

Tsqrt(2pi) exp(-T^2w^2/2)

29
Q

What happens for Fraunhofer diffraction from 2 slits

A

the rapidly varying double-slit interference pattern is modulated by the single slit diffraction pattern which then functions as an envelope to the whole pattern

30
Q

How can we think of two slit diffraction using the fourier method

A

the two slits are two rect functions

31
Q

what is 𝛽 for multi slit diffraction

A

𝛽 = πœ‹π‘ sin πœƒ/πœ†

32
Q

When the slit separation is a, what is 𝛼 for multislit diffraction

A

𝛼 = πœ‹π‘Ž sin πœƒ/πœ†

33
Q

For 2 slit diffraction, with slit width b and separation a, what happens when a=b

A

the 2 slits become a single slit of width 2b

34
Q

In diffraction patterns when does a missing order appear?

A

When the minimum of the single slit diffraction pattern overlaps a maximum of the multi slit interference

35
Q

in terms of a and 𝛼, what are the conditions for missing orders

A

π‘Ž = (𝑝/π‘š) 𝑏 or 𝛼 = (𝑝/π‘š) 𝛽

36
Q

Considering N long narrow parallel slits of width d and centre to centre separation a, how do we find the diffraction pattern

A

integrate over one slit N times

37
Q

What is the N slit diffraction pattern

A

I(πœƒ) = 𝐼0(sin^2 𝛽/𝛽^2)^2 (sin 𝑁𝛼/sin 𝛼)^2
where I0 is the flux density in the normal direction from any slit

38
Q

What is I(0) for multislit diffraction

A

N^2I(0)

39
Q

For multislit diffraction, when do principle maxima occur

A

alpha = 0, Β±pi, Β±pi, … or, equivalently, when π‘Ž sin πœƒπ‘š = π‘šπœ†, π‘š = 0, Β±1, Β±2

40
Q

What is a diffraction grating

A

an N slit device where N is very large and a/d is small

40
Q

How many subsidary maxima are seen in the N slit diffraction pattern

A

N-2

40
Q

How can we think of an N slit as a convolution

A

a convolution of a single slit with N delta functions

41
Q

Describe diffraction from a rectangular aperture

A

The diffracted field is a sinc in x and y because the fourier transform of a rect function is a sinc

42
Q

Describe diffraction from a circular aperture

A

it yields a diffracted airy pattern involving the bessel function Jn(u)

43
Q

What is the radius of the airy disc

A

1.22Rπœ†/2a
R is dist to screen
a is aperture radius