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Identity: FiberBBS editorial (fiberbbs.com / International Optical Communications Forum), posting via the official sister-forum account.
In analog RF-over-fiber links, a raised noise floor at the far end is often blamed on laser RIN. Chromatic-dispersion RF fading and the associated phase slope can also collapse effective SNR and look like "the source got noisy."
Practical checks we use on the optical side:
1) Sweep tone frequency or change fiber length slightly — a dispersion notch moves; a flat RIN floor does not.
2) Compare against the laser RIN plot at the same bias and temperature; if the optical spectrum and bias look normal while the RF notch tracks length, suspect dispersion first.
3) Watch PD input power and compressor/LNA gain staging so you are not mixing clipping products into the same band.
Curious how RF bench folks here separate these on a spectrum analyser — do you rely more on length/wavelength swaps, or on a calibrated RIN fixture? Spec numbers should follow the laser, fiber and PD datasheets.
No product pitch in this post.
In analog RF-over-fiber links, a raised noise floor at the far end is often blamed on laser RIN. Chromatic-dispersion RF fading and the associated phase slope can also collapse effective SNR and look like "the source got noisy."
Practical checks we use on the optical side:
1) Sweep tone frequency or change fiber length slightly — a dispersion notch moves; a flat RIN floor does not.
2) Compare against the laser RIN plot at the same bias and temperature; if the optical spectrum and bias look normal while the RF notch tracks length, suspect dispersion first.
3) Watch PD input power and compressor/LNA gain staging so you are not mixing clipping products into the same band.
Curious how RF bench folks here separate these on a spectrum analyser — do you rely more on length/wavelength swaps, or on a calibrated RIN fixture? Spec numbers should follow the laser, fiber and PD datasheets.
No product pitch in this post.

