Derive local intensity from complex field addition
A complex amplitude records two real pieces of information: magnitude and phase relative to a reference. For equally polarized waves of the same frequency in the same medium, the detector intensity is proportional to the squared magnitude of the summed field. The common proportionality constant is absorbed into the original normalized units here.
Learning outcome: Reconstruct real and imaginary components before intensity. Compare a complete phase scan with a fixed reading, then change the beam ratio and derive visibility from the observed extrema.
Starting recap
Retain complex amplitude before intensity, definite-integral boundaries, normalization, calibration covariance and unused evidence.
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For r=4 and φ=90°, E=1+2i and I=5. The phase scan ranges from 1 to 9, so V=8/10=0.8. The intensity at this one phase happens to equal the incoherent average, but the remaining phase scan distinguishes them.
Open the experimentPredict
Can the same local intensity arise from a coherent and an incoherent record?
Experiment
Reconstruct real and imaginary components before intensity. Compare a complete phase scan with a fixed reading, then change the beam ratio and derive visibility from the observed extrema.
Sum fields before squaring
Worked teaching model · synthetic values · Original equal-frequency, equally polarized coherent fields E1=1 and E2=sqrt(a) exp(iφ), in one reference impedance. Phase-averaged incoherent intensity is a separate comparison; interference redistributes flux across the complete apparatus.
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The cross term survives only when the phase relation is retained.
Original equal-frequency, equally polarized coherent fields E1=1 and E2=sqrt(a) exp(iφ), in one reference impedance. Phase-averaged incoherent intensity is a separate comparison; interference redistributes flux across the complete apparatus.
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 |
|---|---|---|
| Real field component | 1.00000 | amplitude |
| Imaginary field component | 2 | amplitude |
| Coherent local intensity | 5 | relative intensity |
| Incoherent phase-averaged comparison | 5 | relative intensity |
| Maximum over phase | 9 | relative intensity |
| Minimum over phase | 1 | relative intensity |
| Fringe visibility | 0.800000 | ratio |
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The cross term survives only when the phase relation is retained.
Original equal-frequency, equally polarized coherent fields E1=1 and E2=sqrt(a) exp(iφ), in one reference impedance. Phase-averaged incoherent intensity is a separate comparison; interference redistributes flux across the complete apparatus.
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Change to equal beams r=1. Find intensities at 0° and 180°, visibility and the phase average.
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