Integrate a spectrum to predict a fringe envelope
Two delayed copies of one source can retain coherence at each frequency while different frequency components average incoherently in the detector. The relevant calculation averages the phase-dependent cross term over the power spectrum; it does not first add unrelated spectral fields as though all frequencies had a fixed common phase.
Learning outcome: Integrate the real and imaginary spectral terms independently, compare them with the analytic sinc, and distinguish intensity at a delay from a phase-scan visibility.
Starting recap
Retain complex amplitude before intensity, definite-integral boundaries, normalization, calibration covariance and unused evidence.
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With B=2 and τ=0.25, the envelope is 2/π≈0.636620 and the central phase is 5π. Thus μ is negative real and the equal-beam intensity is about 0.726760, while contrast is positive 0.636620. First-zero delay is 0.5.
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Does a zero at one delay mean that the two copies can never interfere at another delay?
Experiment
Integrate the real and imaginary spectral terms independently, compare them with the analytic sinc, and distinguish intensity at a delay from a phase-scan visibility.
Integrate a flat spectral band
Worked teaching model · synthetic values · Original uniform power spectral density on ν0±B/2, ν0=10 inverse time units. Two equal-intensity delayed replicas share each frequency; different frequencies average incoherently over the detector record. μ(τ)=exp(i2πν0τ)sinc(πBτ); first-zero coherence delay is a declared convention.
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Integrating spectral phase yields a signed sinc and an absolute-value contrast envelope, not a universal sharp coherence cutoff.
Original uniform power spectral density on ν0±B/2, ν0=10 inverse time units. Two equal-intensity delayed replicas share each frequency; different frequencies average incoherently over the detector record. μ(τ)=exp(i2πν0τ)sinc(πBτ); first-zero coherence delay is a declared convention.
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 |
|---|---|---|
| Signed envelope factor | 0.636620 | ratio |
| Visibility envelope | 0.636620 | ratio |
| Real normalized coherence | -0.636620 | ratio |
| Imaginary normalized coherence | 3.89817e-16 | ratio |
| Equal-beam intensity at this delay | 0.726760 | relative intensity |
| First-zero delay convention | 0.500000 | time units |
Virtual original records only. No laser, intense-light source, instrument alignment, physical apparatus operation or completed practical competence is supplied.
Integrating spectral phase yields a signed sinc and an absolute-value contrast envelope, not a universal sharp coherence cutoff.
Original uniform power spectral density on ν0±B/2, ν0=10 inverse time units. Two equal-intensity delayed replicas share each frequency; different frequencies average incoherently over the detector record. μ(τ)=exp(i2πν0τ)sinc(πBτ); first-zero coherence delay is a declared convention.
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Use B=1 and τ=0.5, then compare τ=1.
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