Wave optics: Diffraction(2)

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Continuation of the diffraction stuff froms sem 1

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46 Terms

1
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What is the mathematical form for the diffraction pattern from a circular aperture?

  • J1(z)= the Bessel function of the first kind of order 1

  • D= the diameter of the hole

  • θ= the diffraction angle

  • λ= the wavelength of light.

<ul><li><p>J<sub>1</sub>(z)= the Bessel function of the first kind of order 1</p></li><li><p>D= the diameter of the hole</p></li><li><p>θ= the diffraction angle</p></li><li><p>λ= the wavelength of light.</p></li></ul><p></p>
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What is the mathematical form for the diffraction pattern from a 1-D slit?

  • h= the width of the apeture

  • θ= the diffraction angle

  • λ= the wavelength of light

<ul><li><p>h= the width of the apeture</p></li><li><p>θ= the diffraction angle</p></li><li><p>λ= the wavelength of light</p></li></ul><p></p>
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What are the similarities between diffraction by a circular aperture and a 1-D slit?

1. D and h are both simply the width of the aperture in each case.

2. So the denominators and overall-squaring are the same.

3. So we just need to compare the Bessel function to the sine.

<p>1. D and h are both simply the width of the aperture in each case. </p><p>2. So the denominators and overall-squaring are the same. </p><p>3. So we just need to compare the Bessel function to the sine.</p>
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What does the plot of the Bessel function (J1(z)) look like?

  • The function is oscillatory and odd like sine

  • It's not periodic and the extrema decrease with increasing z.

  • For small z the ratio J1(z)/z is finite (in this case, ½) like sinc

  • The first positive zero of the function is at z = 3.832.

<ul><li><p>The function is oscillatory and odd like sine</p></li><li><p>It's not periodic and the extrema decrease with increasing z.</p></li><li><p>For small z the ratio J<sub>1</sub>(z)/z is finite (in this case, ½) like sinc</p></li><li><p>The first positive zero of the function is at z = 3.832.</p></li></ul><p></p>
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<p>What does a diagram of the Airy pattern look like( a Fraunhofer diffraction pattern from a circular aperture)?</p>

What does a diagram of the Airy pattern look like( a Fraunhofer diffraction pattern from a circular aperture)?

  • It is circularly-symmetric

  • It has a large central spot (the Airy disc) surrounded by faint rings.

  • The Airy disc is bounded by the first zero of I(θ)

<ul><li><p>It is circularly-symmetric</p></li><li><p>It has a large central spot (the Airy disc) surrounded by faint rings.</p></li><li><p>The Airy disc is bounded by the first zero of I(θ)</p></li></ul><p></p>
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What is the Airy disc?

  • The bright central spot in the Airy pattern.

  • Its boundary is defined by the first zero of the intensity function I(θ), which marks the location of the first dark ring.

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<p>What is the formula that represents the first dark ring of an airy disc?</p>

What is the formula that represents the first dark ring of an airy disc?

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Why do lenses form finite-size Airy-pattern images of stars?

  • Lenses themselves act as diffracting apertures.

  • When light passes through the lens, it diffracts and forms a finite-size Airy pattern

  • This results in the image of a point-like star being spread out instead of a sharp point.

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<p>What happens when two stars, which are a small angle θ apart, are viewed through a telescope with a small aperture?</p>

What happens when two stars, which are a small angle θ apart, are viewed through a telescope with a small aperture?

  • Their Airy patterns will overlap.

  • Since the Airy patterns(θAiry) are larger than the separation between the stars(θ), they appear as a single object and are unresolved.

<ul><li><p>Their Airy patterns will overlap.</p><p></p></li><li><p>Since the Airy patterns(θ<sub>Airy</sub>) are larger than the separation between the stars(θ), they appear as a single object and are unresolved.</p></li></ul><p></p>
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How can you resolve closely spaced stars in a telescope?

  • You need a larger aperture for the telescope.

  • A bigger aperture reduces the size of the Airy disc making it possible to separate the two diffraction patterns and clearly distinguish the stars.

<ul><li><p>You need a larger aperture for the telescope.</p><p></p></li><li><p>A bigger aperture reduces the size of the Airy disc making it possible to separate the two diffraction patterns and clearly distinguish the stars.</p></li></ul><p></p>
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Does magnification help in resolving closely spaced stars?

No

  • Both the diffraction pattern (θAiry) and the separation between the stars (θ) are magnified by the same factor

  • Therefore the stars still appear unresolved.

<p>No</p><ul><li><p>Both the diffraction pattern (θ<sub>Airy</sub>) and the separation between the stars (θ) are magnified by the same factor</p><p></p></li><li><p>Therefore the stars still appear unresolved.</p></li></ul><p></p>
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What is the Rayleigh criterion definition?

Two incoherent point sources are just resolved if the centre of one's Airy disc falls on the first minimum of the other's.

<p>Two incoherent point sources are just resolved if the centre of one's Airy disc falls on the first minimum of the other's.</p>
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What is the condition for two sources to be resolved according to the Rayleigh criterion?

Two sources are resolved if their angular separation θ is greater than or equal to the angular radius of the Airy disc θAiry

<p>Two sources are resolved if their angular separation θ is greater than or equal to the angular radius of the Airy disc θ<sub>Airy</sub></p>
14
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What factors can make optical instruments perform worse than the Rayleigh criterion?

Factors such as:

  • Optical aberrations

  • Manufacturing errors

  • Atmospheric effects (called "seeing" in astronomy)

15
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What is the point spread function (PSF)?

  • It describes how an optical instrument responds to light from a point source.

  • If the PSF is larger than the Airy pattern, the instrument will not be able to resolve objects as sharply as the Rayleigh criterion predicts.

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What does it mean for an instrument to be "diffraction-limited"?

  • An instrument is diffraction-limited if its resolution is only restricted by the laws of physics,

  • This happens when the instrument is free from aberrations, errors, and atmospheric effects.

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What is the aperture function for Young's double-slit experiment?

The aperture function treats the two slits as a single compound aperture,

<p>The aperture function treats the two slits as a single compound aperture,</p>
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What is the formula for the intensity distribution in Young's double-slit experiment?

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What does the diagram of the intensity distribution in Young's double-slit experiment look like?

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What determines the interference fringes in Young's double-slit experiment?

  • The separation d of the two slits.

  • These fringes are spaced based on the path difference between light from the two slits.

<ul><li><p>The separation d of the two slits. </p></li></ul><p></p><ul><li><p>These fringes are spaced based on the path difference between light from the two slits.</p></li></ul><p></p>
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What determines the diffraction envelope in Young's double-slit experiment?

  • The width h of the individual slits.

  • the width hhh of the individual slits. It represents the overall spread of the light from each slit.It represents the overall spread of the light from each slit.

<ul><li><p>The width h of the individual slits. </p><p></p></li><li><p>the width hhh of the individual slits. It represents the overall spread of the light from each slit.It represents the overall spread of the light from each slit.</p></li></ul><p></p>
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Why are the interference fringes more compact than the diffraction envelope?

The separation d between the slits must be larger than the slit width h (d>h) for distinct interference patterns to form.

<p>The separation d between the slits must be larger than the slit width h (d&gt;h) for distinct interference patterns to form.</p>
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<p>How does decreasing the slit separation d affect the fringe spacing?</p>

How does decreasing the slit separation d affect the fringe spacing?

Decreasing the slit separation d increases the spacing between the interference fringes.

24
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<p>What does increasing N in a multi-slit setup result in?</p>

What does increasing N in a multi-slit setup result in?

Sharper interference maxima.

25
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<p>What is the width of each slit in a multi-slit experiment represented by?</p>

What is the width of each slit in a multi-slit experiment represented by?

h

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<p>What is the center-to-center distance between adjacent slits represented by?</p>

What is the center-to-center distance between adjacent slits represented by?

d

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<p>How is the position of slit p (where p=0 to N−1) defined?</p>

How is the position of slit p (where p=0 to N−1) defined?

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<p>How do you define the edges of a slit at position x<sub>p</sub>​?</p>

How do you define the edges of a slit at position xp​?

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<p>What does the compound aperture function a(x) describe?</p>

What does the compound aperture function a(x) describe?

The overall shape and distribution of the slits.

30
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<p>What is the equation for diffraction angles?</p>

What is the equation for diffraction angles?

  • d= the slit separation

  • m= the diffraction order

  • λ= the wavelength.

<ul><li><p>d= the slit separation</p></li><li><p>m= the diffraction order</p></li><li><p>λ= the wavelength.</p></li></ul><p></p>
31
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Why do diffraction gratings work for spectroscopy?

Because the diffraction angles θ of the m≠0 orders depend on wavelength λ, allowing different wavelengths to be separated.

32
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What happens to diffraction orders as the number of slits (N) increases?

The orders become much narrower, leading to higher resolution.

33
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What is the zeroth-order (m=0) diffraction peak?

The central peak where all wavelengths constructively interfere at θ=0

<p>The central peak where all wavelengths constructively interfere at θ=0</p>
34
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How do diffraction gratings differ from many-slit apertures?

Gratings are usually reflective, while many-slit apertures are transmissive.

<p>Gratings are usually reflective, while many-slit apertures are transmissive.</p>
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What determines the ability of a diffraction grating to resolve closely spaced spectral features?

The width of diffraction peaks in the intensity function I(θ), which depends on the number of grooves (N).

36
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<p>What is the half-width Δθ of a diffraction peak?</p>

What is the half-width Δθ of a diffraction peak?

The angle range from the peak to the next zero

N= the number of grooves

d = the groove spacing

λ= the wavelength.

<p>The angle range from the peak to the next zero</p><p></p><p>N= the number of grooves</p><p>d = the groove spacing</p><p>λ= the wavelength.</p>
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<p>What equation describes the angle of the m-th diffraction order?</p>

What equation describes the angle of the m-th diffraction order?

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<p>What is the Rayleigh criterion in diffraction gratings?</p>

What is the Rayleigh criterion in diffraction gratings?

  • Two spectral lines are just resolved when their separation is equal to Δθ

  • This means the peak of one lies at the first zero of the other.

<ul><li><p>Two spectral lines are just resolved when their separation is equal to Δθ</p></li></ul><p></p><ul><li><p>This means the peak of one lies at the first zero of the other.</p></li></ul><p></p>
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<p>What is theformula for the resolving power R of a spectrometer?</p>

What is theformula for the resolving power R of a spectrometer?

A higher R means better spectral resolution.

<p>A higher R means better spectral resolution.</p>
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<p>What is the minimum resolvable wavelength difference Δλ?</p>

What is the minimum resolvable wavelength difference Δλ?

m= the diffraction order

N= the number of grooves.

<p>m= the diffraction order</p><p>N= the number of grooves.</p>
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Why is the zeroth-order diffraction peak useless for spectroscopy?

Its angle θ does not depend on wavelength, making it unable to separate different wavelengths.

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Why does more light end up in the zeroth order?

Because it is at the peak of the sinc2 envelope, meaning it receives the most intensity.

<p>Because it is at the peak of the sinc<sup>2</sup> envelope, meaning it receives the most intensity.</p>
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What is a "blazed" diffraction grating?

Its designed to shift the sinc2 envelope peak away from the zeroth order and toward a useful diffraction order.

<p>Its designed to shift the sinc<sup>2</sup> envelope peak away from the zeroth order and toward a useful diffraction order.</p>
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How does blazing improve diffraction efficiency?

It directs more light into a specific diffraction order (often the first order) instead of the zeroth order, enhancing wavelength separation.

<p>It directs more light into a specific diffraction order (often the first order) instead of the zeroth order, enhancing wavelength separation.</p>
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Does blazing change the location of diffraction orders?

No, the diffraction orders remain the same, but the intensity distribution shifts.

<p>No, the <strong>diffraction orders remain the same</strong>, but the intensity distribution shifts.</p>
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