Sum interface phases and the complete reflected series
At a lossless normal-incidence interface the electric-field reflection coefficient is r_ij=(n_i−n_j)/(n_i+n_j). A negative coefficient is a π phase reversal; a positive coefficient is not. This interface sign is separate from the propagation phase accumulated while a wave traverses a film.
Learning outcome: Track each interface coefficient and round-trip phase separately, then verify the full power sum and both zero-thickness and matched-index limits.
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For d=100 nm and substrate index 1, r12=+0.2 and φ=π. The complete reflectance is about 0.147929 and transmittance 0.852071. At d=0, the same surrounding media give R=0, not the 0.04 reflectance of an isolated first interface.
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Can a reflection-phase reversal be replaced by adding an arbitrary geometric path length in every surrounding medium?
Experiment
Track each interface coefficient and round-trip phase separately, then verify the full power sum and both zero-thickness and matched-index limits.
Separate interface sign and propagation phase
Worked teaching model · synthetic values · Lossless normal-incidence stack n0=1, film n1=1.5, substrate n2=b, vacuum wavelength 600 nm. Real Fresnel field coefficients and all internally reflected beams are summed coherently. No absorption, dispersion, roughness or operating instructions.
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Reflection signs and propagation phase enter different factors; the complete lossless series closes R+T=1.
Lossless normal-incidence stack n0=1, film n1=1.5, substrate n2=b, vacuum wavelength 600 nm. Real Fresnel field coefficients and all internally reflected beams are summed coherently. No absorption, dispersion, roughness or operating instructions.
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 |
|---|---|---|
| First interface field reflection | -0.200000 | amplitude ratio |
| Second interface field reflection | 0.200000 | amplitude ratio |
| Round-trip propagation phase | 3.14159 | radians |
| Total coherent reflectance | 0.147929 | incident power fraction |
| Total coherent transmittance | 0.852071 | incident power fraction |
| Outgoing energy sum | 1.00000 | ratio |
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Reflection signs and propagation phase enter different factors; the complete lossless series closes R+T=1.
Lossless normal-incidence stack n0=1, film n1=1.5, substrate n2=b, vacuum wavelength 600 nm. Real Fresnel field coefficients and all internally reflected beams are summed coherently. No absorption, dispersion, roughness or operating instructions.
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Keep d=100 nm but set substrate index 1.5. What changes?
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