I'm trying to understand a section of a paper. They're talking about the signal generated by a photomultiplier tube when photons from fluorescence are coming into it. The sentence says, "Since the number of photo-electrons ultimately captured by the PMT is finite, the signal quantitation is stochastic with a variance governed by the Poisson
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Poisson processes are defined by only one parameter, lambda, which is both the mean and the variance of the process. So, they're taking advantage of this and saying that the square root of the mean (aka expected number of captured photo electrons) is the same as the square root of the variance (the standard deviation).
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The finiteness of the photons means that you have to amplify the signal. This amplification presumably leads to a Poisson distribution. If you had an infinite/enormous source of photons, you wouldn't need this amplification and could take a (more) direct reading, which would be more or less non-distributed. Or at least that's my guess.
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Are you good with your first set of questions?
Is Q still talking about the PMT? If so, I think it is just saying that if you need fewer photo-electrons to get a measurable signal (fluorescence intensity), there will be more error in the signal because the signal is triggered relatively easily (and could be triggered by stray photons hitting the tube that did not come from your source of interest).
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