The attached plots show 55Fe PH spectra from the PPP at various applied high voltages. I also took a few spectra where the ADC gate width and/or the delay between the start of the gate and the leading edge of most WC signals was varied. The spectra are "named" as follows: PVVVGGDD where: VVV - (HV/10) in volts GG - (adc gate width)/10 in ns DD - delay between gate and signal in ns Most spectra were taken with gate width = 300 ns, and delay = 45 ns. Shortening the gate below ~ 100 ns, and reducing the delay to ~ 0 had effects similar to that shown in P1850800 below. Increasing gate width or delay above 300ns/45ns had no effect. At very low voltages there appears to be only one peak in the spectrum. As the voltage is increased a peak at higher PH appears. As the voltage is further increased, more and more counts fall into the "high" peak as opposed to the "low" peak. The overall gain of the system was varied using the gain control on the NIM spectroscopy amp, and an attenuator box. To enable rough comparisons between spectra, I have written the relative gain (varying from 0.3 to 10) on each of the spectra. Iouri and I are working on an absolute calibration of the gas gain in each case, so that a more careful study of what is happening can occur. It is possible that some kind of streamer mode is occuring. Since the onset of the streamer mode is likely dependent on the density of charge deposited in the WC, we need to do further studies to understand what effects may occur with minimum ionizing electrons and heavily ionizing muons. Robert