Polarization and Modern Optics
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Polarization and Modern Optics
Polarizing Beam-Splitter CubeHalf-wave Plate
Quarter-wave PlateElectro-Optic Modulator
Charles Bernando

Polarization
Property of waves that describes the orientation of their oscillationsExample: electromagnetic wave (light)
φ = phase difference1 0 cos( . )E E k y wt 2 0 cos( . )E E k y wt

Linear Polarization Circular Polarization
φ = 0, ±π, ±2π, .. φ = ±π/2, ±3π/2, ..
Elliptical Polarization
1 0 cos( . )E E k y wt 2 0 cos( . )E E k y wt
1 0 cos( . )E E k y wt
1 0 cos( . )E E k y wt
2 0 0sin( . ) cos .2
E E k y wt E k y wt
2 0 cos( . )E k y wt

Polarizing Beam-splitter Cube• Split randomly polarized beams into 2 orthogonal,
linearly, polarized components (s-polarized & p-polarized). S-polarized is reflected at 900 angle, while P-polarized light is transmitted
• S-wave: electric field perpendicular to plane of incidence• P-wave: electric field parallel to plane of incidence

• AR (antireflection) coating: produce max transmission efficiency
• Cement: bind 2 prisms• BS (beam-splitter) coating or dielectric coating or thin
film coating: consists of thin layers of transparent dielectric materials with different refractive indexes, which are deposited on a substrate. It will produce phase shift due to reflections and reinforce certain wavelengths. By controlling the thickness and number of the layers, the reflectivity & transmissivity can be adjusted

= vector of beam-splitter interface = vector of incident light = state of polarization of s-wave = state of polarization of p-wave
For light incident along z-axis,
J. L. Pezzaniti and R. A. Chipman. Angular dependence of polarizing beam-splitter cubes. Appl. Opt. 33(10), pp. 1916-1929. 1994.
11,0, 1
2n
0,0,1k
n ks
n k
p s k
0,1,0s
1,0,0p
n
k
sp

Half-wave Plate• Shift the phase between 2 perpendicular
components of electric field (the phase shift is π rad)• Change linear polarized wave into another linear
polarized wave• Material: quartz, calcite• Optical axis = fast axis/extraordinary axis is
the axis with the smaller index of refraction• Slow axis = ordinary axis (perpendicular to fast axis)
is the axis with the higher index of refractionThe light component along the fast axis will travel faster than the light component along the slow axis

Due to velocity difference, the light component along fast axis and slow axis will be shifted until the outcome phase shift is π rad. The phase shift depends on the thickness of a material.
φ = phase shiftne = extraordinary index
no = ordinary index
L = thickness of materialλ = wavelength
2 .( ).e on n L

Quarter-wave Plate• Shift the phase between 2 perpendicular components of
electric field (the shift phase is π/2 rad)• Change linear polarized wave into circular polarized
wave when the incident light makes 450 angle with the fast axis

Electro Optic Modulator• A device used for controlling the polarization of a laser
beam with an electrical control signal• By applying an appropriate voltage to the RF input, a
corresponding change in the extraordinary refractive index will occur
• The voltage required for inducing a phase change of π is called the half-wave voltage

Jones Matrix• Linear horizontal polarizer• Linear vertical polarizer• Half wave plate
• Quarter wave plate
Example: linearly polarized light 450 (basis ) is incident on a horizontal polarizer. The outcome is
horizontally polarized
1 0
0 0
0 0
0 1
cos 2 sin 2
sin 2 cos 2
2 2
2 2
cos sin (1 )sin cos
(1 )sin cos sin cos
i i
i i
1 0 1 1
0 0 1 0
1
1
For beam splitter, please see: A. L. Fymat. Jones's matrix representation of optical instruments. I: Beam splitters. Appl. Opt. 10(11), pp. 2499-2505. 1971.

Conclusion• Beam splitter is used to resolve a beam of light
into 2 beams by reflecting the s-wave and transmitting the p-wave
• The wave plates (half and quarter wave plate) are designed to change the state of polarization of incoming light
• The Electro Optic Modulators use a potential difference to change and adjust the extraordinary refractive index to get the expected phase shift between 2 components of light