Cross Polarizers with a wave plate retardation

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SUMMARY

The discussion focuses on the behavior of light passing through a wave plate placed between crossed polarizers. The transmitted intensity is mathematically expressed as I_out/I_in = sin²(2θ) * sin²(τ/2), where τ represents the retardation defined by τ = (η_0 - n_e) * w * L/c. Setting the optical axis at θ = 45° maximizes contrast in practical applications. The solution involves vector addition of electric fields and averaging to determine intensity.

PREREQUISITES
  • Understanding of wave plate retardation and its formula τ = (η_0 - n_e) * w * L/c
  • Familiarity with the principles of polarized light and crossed polarizers
  • Knowledge of electric field representation and vector addition in optics
  • Basic grasp of intensity calculations in wave optics, specifically I = E * E*
NEXT STEPS
  • Research the effects of varying the angle θ on transmitted intensity through polarizers
  • Study the mathematical derivation of intensity equations involving wave plates
  • Explore practical applications of wave plates in optical devices
  • Learn about different types of polarizers and their characteristics in optical systems
USEFUL FOR

Students and professionals in optics, physicists studying light behavior, and engineers designing optical systems will benefit from this discussion.

jcbale1
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Homework Statement


"Consider a wave plate with a retardation τ=(η_0-n_e)*w*L/c. Show that when it is placed between crossed polarizers with its optical axis at an angle of θ with respect to the polarizer axis, the transmitted intensity is given by:

I_out/I_in= (sin^2(2θ)(sin^2(τ/2))

In practice, one often sets the optical axis at θ=45° to obtain maximum contrast.


Homework Equations




E=P_θ*P_0*E_0


I=E times E*


The Attempt at a Solution



I know that without any retardation I/I_0=cos^2(θ). I'm really not sure how to approach this problem
 
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Let's start by rewriting your given equations:

ψ = (n_o - n_e)Lω/c

since ψ is a radian angle so τ is not a good symbol since it usually has dimensions of time.

Then Io/Ii = sin2(2θ)sin2(ψ/2)

So you have one sinusoidally time-varying electric vector field Eo that passes thru the plate and then thru the polarizer and analyzer, and a second field Ee that does the same but is phase-shifted by ψ radians w/r/t Eo and is perpendicular to it.

Then at the output of the analyzer, add the two fields vectorially, then square and time-average to get the intensity, & off you go.
 
Thank you very much, that helps a lot!
 

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