Reflection and transmission I Polarization plays an important role - - PowerPoint PPT Presentation

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Reflection and transmission I Polarization plays an important role - - PowerPoint PPT Presentation

Reflection and transmission I Polarization plays an important role in reflection and transmission at the interface between two media (1) (3) Medium 1 (2) Medium 2 || = y and = x and angles are referenced with respect to normal of


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SLIDE 1
  • P. Piot, PHYS 630 – Fall 2008

Reflection and transmission I

  • Polarization plays an important role in

reflection and transmission at the interface between two media || = y and ⊥ = x and angles are referenced with respect to normal

  • f the interface.
  • Note Snell’s law:

Medium 1 Medium 2 (1) (3) (2)

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SLIDE 2
  • P. Piot, PHYS 630 – Fall 2008

Reflection and Transmission II

  • We write
  • Boundaries condition on E and B gives

(Fresnel equations)

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SLIDE 3
  • P. Piot, PHYS 630 – Fall 2008

TE (or s) polarization

  • External reflection (n1<n2)
  • Internal reflection (n1>n2)

θ1(deg) Arg(rx) |rx| θ1(deg) Arg(rx) |rx|

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SLIDE 4
  • P. Piot, PHYS 630 – Fall 2008

TM (or p) polarization

  • External reflection (n1<n2)
  • Internal reflection (n1>n2)

θ1(deg) Arg(rx) |rx| θ1(deg) Arg(rx) |rx| Brewster angle

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SLIDE 5
  • P. Piot, PHYS 630 – Fall 2008

Optics in anisotropic crystals

  • A dielectric medium is said to be anisotropic if its optical properties

depends on the direction

  • Anisotropy depends on the crystal structure

– If molecules randomly located in space and are isotropic (or

  • riented along random directions) the medium is isotropi (gases,

liquid and amorphous solids) – If the structure takes the form of disjoined crystalline grains randomly oriented, the crystal is a polycrystalline and is in general anisotropic – If the molecules are organized in space according to a regular perioc pattern and oriented in the same direction, as in crystals, the medium is in general anisotropic

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SLIDE 6
  • P. Piot, PHYS 630 – Fall 2008

Permittivity tensor

  • Only anisotropy is considered
  • The polarization and dielectric displacement are now given by

and wherein χ is a tensor (= a 3x3 array)

Ex Ey Ez Px Py Pz

χ11 χ21 χ31 χ12 χ22 χ32 χ13 χ23 χ33

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SLIDE 7
  • P. Piot, PHYS 630 – Fall 2008

Principal axes

  • The elements of the permittivity tensor depend on the choice of

coordinate system

  • However a coordinate system can be found such that the tensor is

diagonal i.e.

  • This coordinate system define the principal axes and principal planes

associated to the crystal.

  • The corresponding refractive indexes are known as principal

indexes.

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SLIDE 8
  • P. Piot, PHYS 630 – Fall 2008

Biaxial, Uniaxial & isotropic crystal

  • Crystals with three different principal refractive indexes are referred

to as biaxial crystals

  • Crystal with two different principal refractive indexes are referred to

as uniaxial crystals

  • For uniaxial crystals, the refractive indexes are n1=n2=no, and n3=ne

where “o” stands for ordinary axis and “e” for extraordinary axis.

  • If no>ne the crystal is said to be a positive uniaxial crystal