Use complex projections and test the order of optical elements
The introductory Jones extension represents a fully polarized monochromatic field by two complex components. The original normalized input is E=(1,exp(iδ))/sqrt2, so |Ex|²+|Ey|²=1. Relative phase changes the polarization state even though each component intensity remains one half.
Learning outcome: Carry real and imaginary components through each projection, compare both orders and explain why a changed relative phase alters the result despite unchanged component intensities.
Starting recap
Retain complex amplitude before intensity, definite-integral boundaries, normalization, calibration covariance and unused evidence.
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Try
For δ=90° and θ=45°, the first analyzer transmits 0.5 and the second gives 0.25. Reversing the order also gives 0.25 for this particular input. With δ=0° at the same angle, forward order gives 0.5 while reversed order still gives 0.25.
Open the experimentPredict
Does equal output for one input prove that two optical transformations commute?
Experiment
Carry real and imaginary components through each projection, compare both orders and explain why a changed relative phase alters the result despite unchanged component intensities.
Preserve relative phase and polarizer order
Worked teaching model · synthetic values · Original fully polarized normalized Jones vector (1,exp(iδ))/sqrt2. Ideal linear polarizer Pθ=uθuθᵀ followed by horizontal P0, compared with reversed order. Monochromatic Jones extension; not a description of unpolarized light or every partially coherent source.
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A complex two-component input retains phase; sequential projection matrices generally do not commute.
Original fully polarized normalized Jones vector (1,exp(iδ))/sqrt2. Ideal linear polarizer Pθ=uθuθᵀ followed by horizontal P0, compared with reversed order. Monochromatic Jones extension; not a description of unpolarized light or every partially coherent source.
The vertical axis is rescaled to this case’s actual range; equal display height does not imply equal optical power. The finite curve is illustrative; the ledger preserves the exact case values and stated numerical quadrature.
| Quantity | Value | Unit |
|---|---|---|
| Input intensity | 1 | ratio |
| After angled first polarizer | 0.500000 | input fraction |
| Angled then horizontal intensity | 0.250000 | input fraction |
| Horizontal then angled intensity | 0.250000 | input fraction |
| Order-dependent difference | 0 | input fraction |
Virtual original records only. No laser, intense-light source, instrument alignment, physical apparatus operation or completed practical competence is supplied.
A complex two-component input retains phase; sequential projection matrices generally do not commute.
Original fully polarized normalized Jones vector (1,exp(iδ))/sqrt2. Ideal linear polarizer Pθ=uθuθᵀ followed by horizontal P0, compared with reversed order. Monochromatic Jones extension; not a description of unpolarized light or every partially coherent source.
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Set δ=180° and θ=45°. Compare the two orders.
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