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|    sci.optics    |    Discussion relating to the science of op    |    12,750 messages    |
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|    Message 12,159 of 12,750    |
|    Robert Baer to Phil Hobbs    |
|    Re: Third order IMD in photomultipliers-    |
|    18 Nov 15 22:33:51    |
      XPost: sci.electronics.design       From: robertbaer@localnet.com              Phil Hobbs wrote:       > I'm working on an interesting project for a biotech customer, and I       > could use some wisdom from the assembled multitude.       >       > They're building a scanning fluorescence microscope that scans several       > lines at once with a single photomultiplier, using a clever scheme to       > make each line come out at a different RF frequency.       >       > The frequencies are inherently evenly spaced, so third-order IM products       > cause image artifacts. So they asked me to come up with a way to reduce       > the IMD.       >       > I've been doing some measurements, and have found the usual cubic       > dependence of the IM3 products up above about 50 uA of anode current.       > That's generally a combination of voltage sag in the dynode bias string,       > plus some space-charge effects. It can be reduced by changing the       > dynode voltage distribution so that the last few stages have more bias.       >       > Interestingly, though, below ~50 uA there's a broad range of anode       > currents (20 dB or so) where the IM3 products go up linearly with the       > signal, so that the SFDR is a nearly constant 60 dB, plus or minus a       > few. This is without changing ranges on the spectrum analyzer or       > anything like that.       >       > Ahah, you say, the IM3 is in the illumination source, which runs at a       > constant drive level. So I thought, but it ain't so.       >       > My illumination source is a pair of blue LEDs, each driven from a       > separate amp with separate power supplies. To get the spurs big enough       > to see, I'm using two synthesizers locked together--one is just a       > frequency doubler hung off my 10 MHz rubidium reference, and the other       > is a PTS1000 locked to the same reference, running at 20.001 MHz. The       > analyzer is an HP 8566B, locked to the same reference. That way I can       > use a 10-Hz resolution bandwidth to see the spurs.       >       > Using a photodiode, I've verified that the spurs in the light sources       > are below -80 dBc.       >       > There's mention in the literature of a space-charge effect at the       > photocathode, which would vary less with gain than in the last stages.       > If that's it, the -60 dB would be set at the very beginning, so it       > should depend mostly on the actual light intensity at the photocathode.       >       > However, the linear behaviour occurs regardless of whether I'm using a       > fixed light level and adjusting the anode current with the bias voltage       > pot or leaving the voltage alone and using a variable optical attenuator.       >       > It also doesn't depend on the attenuation of the signal in the RX       > chain--adding a 10 dB pad doesn't change the SFDR in that anode current       > range.       >       > This is, in other words, weird as hell.       >       > Any ideas?       >       > Thanks       >       > Phil Hobbs       >        Am too ignorant in that to give direct help, but stupid enough to       give possible "work-around".        Since they have a "clever scheme to make each line come out at a       different RF frequency", have them not harmonically related (like the       DTMF frequencies as used by Ma Bell).        Maybe there is really no such thing as "inherently evenly spaced";       that it just looks that way..              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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