Multi-beam Interference Flashcards

1
Q

What is a multi-beam interferometer

A

a spectroscopic device of extremely high resolving power, also serving as a basic laser resonator cavity

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2
Q

What are the priciple components of the Fabry-Perot Interferometer

A

two plane parallel, highly reflecting surfaces, separated by some distance d.

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3
Q

When the refractive index outside the fabry-perot slab is different from that inside what is the path difference

A

2nd cosπœƒ, but due to one of the reflections happening at a denser medium, there is an additional pi phase change so overall pd between 2 rays is 2nd cosπœƒ - Ξ»/2

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4
Q

(in words) what is the fraction of intensity reflected of a fabry perot interferometer

A

energy carried by reflected [transmitted] wave/energy carried by incident wave

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5
Q

How does a Fabry-Perot etalon work?

A

By constructive interference of radiation from multiple reflections between two exactly parallel surfaces with a gap between them. The plates are coated with a reflective inner surface.
Mechanically varying the gap by moving the mirrors makes it an interferometer

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6
Q

Describe the optical set up to observe interference from a Fabry-Perot Interferometer

A
  • incident beam goes into the slab
  • each ray, reflected or transmitted bears a fixed phase relationship to all the other rays
  • phase differences arise from optical path length differences and phase shifts at certain reflections
  • coherent waves are brought to a focus by lenses on either side of the slab where they interfere
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7
Q

For a Fabry-Perot interferometer what are the optical path length differences and phase differences between adjacent rays

A

Ξ› = 2𝑛𝑑 cos πœƒ
𝛿 = 2πœ‹ (2𝑛𝑑 cos πœƒ)/πœ†

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8
Q

What type of fringes does the Fabry-perot form

A
  • fringes of equal inclination
  • formed at infinity and observed using a converging lens
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9
Q

What function describes the ratio of transmitted intensity to the incident intensity

A

the Airy Function

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10
Q

What formula defines the contrast/coefficient of finesse

A

F = 4R/(1-R)^2

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11
Q

What is the condition for interference peaks?

A

mπœ† =2nd cosπœƒ

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12
Q

Define the free spectral range

A

the frequency spacing between orders of the Fabry-Perot cavity
the repetition frequency of the spectrum

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13
Q

What is the formula for the FSR or the frequency spacing?

A

c/2nd

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14
Q

What is the Finesse of a cavity

A

the finesse of a cavity defines the fringe sharpness and depends on the reflectivity of the cavity mirrors

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15
Q

what is the formula for the finesse

A

pi*sqrt(F)/2

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16
Q

How is the FWHM bandwidth related to the finesse and what does this imply

A

it is inversely proportional
implies that high finesse = sharper fringes

17
Q

How does multibeam compare to 2 beam interference

A

multibeam redistributes the energy density

18
Q

How does multibeam interference allow us to see closely spaced wavelengths

A

high resolution can be achieved by adding together radiation from many coherent sources
sharper fringes give a higher resolution so we can see closely spaced wavelengths in the interference pattern

19
Q

How can you achieve a higher resolution of the fabry perot

A

By operating at a higher order number at the expense of smaller fsr

20
Q

what is the ultimate limit on finesse

A

the flatness of the mirrors

21
Q

What is one of the main challenges of the F-P

A

it is very difficult to change mirror separation while maintaining parallelism of plates

22
Q

What are the commercial uses of the F-P

A
  • mode analysis of diode lasers
  • optical cavities or resonators for lasers
23
Q

Uses of thin dielectric film coatings

A
  • elimination of unwanted reflections from glass surfaces
  • multiplayer, nonabsorbing beamsplitters
24
Q

Describe how antireflection coatings work

A
  • using the boundary conditions at the interface, we can show that at very close to normal incidence, the reflectance formula simplifies for a particulat film thickness and refractive index relationship
25
Q

How do interference filters work

A
  • like a thin F-P etalon
  • if plate separation in order of a wavelength, peaks are widely separated
  • all but one peak can be blocked using an absorbing filter
  • transmitted light corresponds to a single sharp peak
  • etalon serves as a narrow band-pass filter
26
Q

What are the conditions for interference to occur

A
  • waves have the same wavelength and polarisation
27
Q

If wavelengths and polarisations are the same, what is the irradiance of the interference of 2 waves

A

𝐼 = 𝐼1 + 𝐼2 + π‘πœ–Re{π‘¬πŸ βˆ™ π‘¬πŸβˆ— }

28
Q

If two waves combine but cannot interfere, what is the irradiance

A

I = I1 + I2

29
Q

What are the Fresnel-Arago Laws for Interference of polarised light

A
  • orthogonal coherent polarisation states cannot interfere
  • parallel coherent polarisations will interfere like natural light
  • 2 constituent orthogonal polarisation states of natural light cannot interfere to form a readily observable fringe pattern even if rotated into alignment because they are incoherent