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SCIENCE · INVESTIGATE AND EXPLAIN

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

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.

01800.5000000linear analyzer angle (degrees)transmitted fraction

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.

Original conditional optical ledger
QuantityValueUnit
Input intensity1ratio
After angled first polarizer0.500000input fraction
Angled then horizontal intensity0.250000input fraction
Horizontal then angled intensity0.250000input fraction
Order-dependent difference0input 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.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

1. Establish the optical mechanism

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.

An ideal linear polarizer at angle θ transmits the component along the real unit vector u=(cosθ,sinθ). Its matrix is Pθ=u uᵀ. Thus the transmitted complex amplitude along u is (cosθ+sinθ exp(iδ))/sqrt2, and intensity is [1+sin(2θ)cosδ]/2.

A following horizontal polarizer multiplies that intensity by cos²θ. In the reverse order, the first horizontal polarizer retains intensity one half and removes the original y component; the subsequent angled polarizer gives cos²θ/2. These are generally different because P0Pθ and PθP0 need not commute.

For δ=90°, the ideal input is circularly polarized in the stated phase convention and every linear analyzer transmits half the intensity. That special equality does not make the two matrices commute for arbitrary inputs. A single deterministic Jones vector cannot represent unpolarized light; partially polarized ensembles require a different statistical description. No physical polarizer or light-source procedure is required.

2. Work the original evidence

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.

3. Predict and investigate

Does equal output for one input prove that two optical transformations commute?

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.

Transfer the derivation to a changed case

Set δ=180° and θ=45°. Compare the two orders.

Retain your prediction, intermediate reasoning and assumptions before opening public feedback.

Compare a worked response

The input is linear along the orthogonal diagonal. The angled-first projection is zero, so forward output is zero. Horizontal-first retains 0.5 and the angled projection leaves 0.25.

Primary mechanism context. Checked 31 October 2026. Original prose, records and diagrams; no copied source exercises or physical light-source operation. Retain first reasoning and public-feedback exposure in the course evidence workspace when registered.

Apply

Why is the reversed-order output independent of the original phase δ in this packet?

Public practice checks a specific claim. It does not establish independent mastery.

Set δ=180° and θ=45°. Compare the two orders.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

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