Stochastic Resonance
en.wikipedia.org
en.wikipedia.org
This diagram makes it a lot simpler: https://www.researchgate.net/profile/Sverker_Sikstroem/publi...
The article talks about the white noise resonating with the signal but not the noise. I'm trying to picture white noise as a summation of all frequencies, but I've never thought about the phase of the components. If two signals of the same frequency are in phase then they resonate, but if they are out of phase they cancel each other out. What does the phase of the components look like in white noise?
After that, filter out unimportant frequencies and return the volume to normal.
The important data isn't the volume necessarily, but the specific frequency and tempo.
The article points out that with too much noise, this does not work.
[0] http://www.scholarpedia.org/article/Stochastic_resonance#His...
On this article they describe it as a phenomenon of bistable systems. The noise enables the oscillation.
Which bit of this doesn't apply?
What makes white noise interesting is that it has a zero DC component (on average) by randomly adding energy as often as it subtracts, while passing through analog components (like a capacitors where R(s) = 1/(sC) in s-domain). In my view, this is still a form of amplification.
Adding Gaussian noise around your source frequency is certainly source amplification because it's equivalent to attenuating the surrounding "noisy" frequencies for the benefit of your sensor equipment. This would increase the signal-to-noise ratio, but you have to know what the base frequency is you are trying to measure.
I hope to be corrected by the signal folks, but it seems misleading to me that "the frequencies in the white noise corresponding to the original signal's frequencies will resonate with each other," when resonance does not occur in the signal, but in the resonant body of the sensor, and so this is more about sensor system calibration than boosting an unknown source signal.
It seems that the practical implications are that you can have simpler sensors (that work in a narrower band) if you can cheaply control the input noise based on sensor reading.
For those interested in reading more, this article (on stochastic resonance's potential importance in biological sensing) is edifying: https://www.physik.uni-augsburg.de/theo1/hanggi/Papers/282.p... (Hänggi, Peter. "Stochastic resonance in biology: how noise can enhance detection of weak signals and help improve biological information processing." ChemPhysChem 3.3 (2002): 285-290.)
(Perhaps this is an example of how biological systems can value accurate sensation so highly that they invent ingenious sensing schemes to achieve high performance.)
But that only works if your signal (including the measurement circuit) is not rock steady, which would make both samples identical and so you don't gain any information. Adding noise helps the samples be different which can increase the effective resolution. If you were just on the brink of a discretization bucket, a kick of noise will likely push you into the next bucket
Dithering exploits the human senses, so maybe in a way it is the same thing, just for the meatware in our heads.
Not sure what distinction you are making between inverse and reverse, but I'm curious.
The idea isn't very complicated, but the Wikipedia explanation is god-awful. I'll try: You modulate the cause of the signal you want to measure with some sine function of frequency f. Then you take the resulting signal and multiply it with the clean sine function of frequency f. You integrate (sum up) the result of that over a long time. Incredible sensitivity (and very slow reaction to changes) results.
If you know what a convolution is, the explanation can be shorter.