please use the new report guidelines!courses.washington.edu/phys331/xu/2015/lecture_3-2015.pdf ·...

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Summary of lab reports Your reports are awesome! Units (hand written data sheets) Always include your own raw data in the report Partner’s name Organized data sheet/neat hand writing Label the parameters in the figure Error analysis (understand what you reported) New reports are due next week. Please use the new report guidelines!

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Page 1: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Summary of lab reportsYour reports are awesome!

Units (hand written data sheets) Always include your own raw data in the report Partner’s name Organized data sheet/neat hand writing Label the parameters in the figure Error analysis (understand what you reported)

New reports are due next week.

Please use the new report guidelines!

Page 2: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

Broad Applications: laser wave meter; Raman spectrometer; Ultra-narrow bandwidth laser; optical filters etc….

M2

detector

o

1l

2l

1E

2E

M1

Michaelson interferometer

Page 3: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

λ

r (distance)

Wave Propagation of Light

𝐸 = 𝐴𝑒𝑖𝑘.𝑟

𝑘 =2𝜋

𝜆

r= ro + m λ 𝐸 𝑟 = 𝐴𝑒𝑖 𝑘.𝑟𝑜+𝑘𝑚𝜆

= 𝐴𝑒𝑖𝑘.𝑟𝑜𝑒𝑖2𝑚𝜋 = 𝐸(𝑟𝑜)

Page 4: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

M2

detector

o

1l

2l

1E

2E

M1

Constructive Interference

𝐸 = 𝐴𝑒𝑖𝑘.𝑙

l2= l1 + 2d

If 2d= mλ

Phase difference δ = 𝑘. 2𝑑 = 2𝑚𝜋

Page 5: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Quiz!

M2

detector

o

1l

2l

1E

2E

M1

Initially, M2 at position do, and it is a dark circle in the middle.

(1)M2 moves by ¼ λ. Is the center bright or dark?

(2) M2 moves by ½ λ. Is the center bright or dark?

Page 6: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Quiz!

M2

detector

o

1l

2l

1E

2E

M1

Initially, M2 at position do, and it is a dark circle in the middle.

(1)M2 moves 7 μm. The center changes from dark to dark 20 times. What is the exciton laser wavelength?

Page 7: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

r: reflection coefficientt: transmission coefficient

ConstructiveInterference

when 2dcosq = nl

OA

B

M1M2

OA+AB=OA (1+cos2θ)=2𝑐𝑐𝑜𝑠2 𝜃 𝑂𝐴

=2𝑐𝑐𝑜𝑠2 𝜃 𝑑

cos θ=2dcos(θ)

Eot’

Eot’r

Eot’rr’

Eot’r2r’

Page 8: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

Hecht, Pg 422, Eq. 9.65

If there is no absorption, ( )t

o

IA

Iq

-

Page 9: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

Coefficient of finesse

R~0.99->F~40,000 cos

4 dq

l

γ

Page 10: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

cos4 d

q

l

Resolving power of instrument ~ frequency width of peaks

Hecht, Pg 423, Fig. 9.45Fabry-Perot fringes for (monochromatic light)

γ

Page 11: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer4 d

l

Free spectral range

2m 2( 1)m

same l4 d

l

4 'd

l ' / 2d d l

Central spot scanning

d

d’

γ

Page 12: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer4 d

l

Free spectral range

2m 2( 1)m

same l4 d

l

4 'd

l ' / 2d d l

4 d

l

4

'

d

lDifferent l

In this case, we cannot distinguish these two frequencies apart

'l l l Free spectral range

Central spot scanning

γ

Page 13: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot InterferometerFree spectral range

FSRf

4 42( 1) 2

'

d dm

l l

' 1

' 2d

l l

l l

f cl 'l l

2FSR

cf

d

'

'

2 '

( )

1

/ 2

c f f

ff

c ff d

The round-trip time for light travels in the cavity

Page 14: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometerresolving power ~ free spectral range

2 /Finess 4 4d df

c

l

1/2

4 d f

c

FSRf

Finesse

Resolving power: Δf=

f cl

2𝜋

𝛾Δ𝑓 =

𝐶

2𝑑

Page 15: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

Page 16: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

Fabry-Perot Interferometer

Page 17: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r

2FSR

cf

d

FSRf

Finesse

Resolving power:

Page 18: Please use the new report guidelines!courses.washington.edu/phys331/xu/2015/Lecture_3-2015.pdf · λ r (distance) Wave Propagation of Light 𝐸=𝐴 𝑖 . 𝑘= 2𝜋 𝜆 r= r