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Lect 14 Dispersion in Optical Fiber

Jun 03, 2018

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  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    vg (m/s)

    (1/s)

    TE1

    TE2

    2.0810 8

    2.0710 8

    2.0610 8

    2.0510 8

    0 110 15 210 15 31015

    cut-off= 2.31014

    c/n2

    c/n1

    d=10mn1=1.455

    n2=1.440

    n2

    Modal or intermodal)

    dispersion:

    Waveguide can support

    several modes having

    different values of v

    g

    Solution: Use single

    mode waveguide

    Group velocity depends onFrequency: intramodal dispersion

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    Dispersion in single-mode waveguide:

    Group velocity depends on frequency.

    Limitation on data rate and transmission distance.

    t

    Intensity

    Spectrum

    Intensity

    f

    t

    Spread

    Intensity

    Dispersive SMF

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    n

    500 700 900 1100 1300 15001700 1900

    1.44

    1.45

    1.46

    1.47

    1.48

    1.49

    Wavelength (nm)

    Refractive Index for Silica

    - Material or chromatic) dispersion

    Refractive index of any materialdepends on frequency(wavelength)

    vg depends on frequency

    (wavelength)

    Why does single mode waveguide

    have dispersion?

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    Waveguide dispersion

    Even if refractive indexdoes not change,vg depends onfrequency (wavelength)

    dn1

    n2

    n2Why does single mode waveguide

    have dispersion?

    2y

    dX k=

    2

    dY =

    2

    2

    2 2 2 2 2

    0 1 2( )2

    dX Y k n n

    + =

    tanY X X=

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    Waveguide dispersion

    Even if refractive index

    does not change,vg depends onfrequency (wavelength)

    d=10mn1=1.455

    n2=1.440

    n2

    vg (m/s)

    (1/s)

    TE1

    2.0810 8

    2.0710 8

    2.0610 8

    2.0510 8

    0 110 15 210 15 31015

    14

    c/n2

    c/n1

    Why does single mode waveguide

    have dispersion?

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    Dispersion coefficient, D, for silica fiber with a=4.2mDm: material (chromatic) dispersion only

    Dw: waveguide dispersion only

    Dm+Dw: total dispersion

    0

    1.2 1.3 1.4 1.5 1.61.1

    -30

    20

    30

    10

    -20

    -10

    (m)

    Dm

    Dm+ Dw

    Dw0

  • 8/12/2019 Lect 14 Dispersion in Optical Fiber

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    20

    -10

    -20

    -30

    10

    1.1 1.2 1.3 1.4 1.5 1.6 1.7

    0

    30

    (m)

    Dm

    Dw

    Dch

    = Dm

    + Dw

    1 2

    n

    r

    Thin layer of cladding

    with a depressed index

    D

    It is possible to control D by changing waveguide structure

    Dispersion Flattened Fiber)

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    How do we model dispersion

    0 0

    0

    22

    0 0 2

    2

    0 1 0 2 0

    20

    0

    1( ) ( ) 2

    1 ( ) ( ) ( )

    2

    1 1 1 = ( )( ) 2

    ==> Dispersion exists if is not not linear with

    In Silica

    g gv v

    + = + + +

    + +

    + +

    i i

    i i

    i i

    2

    2

    2

    fiber, 20 ps /km at =1.5 m

    (With 0, increases as increases)gv

    0)

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    High-Speed Circuits and Systems LaboratoryOptoelectronics and Photonics

    Lect 14: Dispersion in Optical Fiber

    Exercises:

    Prob. 8, 9, 10, 14