−Table of Contents
R68 Noise Stability
Noise Width from PSDs
R68 data was taken over several months and in may different operating conditions. This is an analysis of the noise of the -125V data. In that dataset, there were 193 background, 535 Na, and 640 PuBe series included in the final analysis. Each series was 10 min long including randoms.
The PSD of pulse-less randoms was calculated by BatNoise for each series. The resulting PT PSDs were averaged for each data type and are shown below. Interestingly, the Na data, which had the highest rate, appears to have the highest low-frequency noise. This is likely due to more frequent sloped baselines in the pulses. Note that these PSDs are in the same units as PTOFamps, which is to say it is NOT the current through the TES, but something proportional to it due to incorrect factors in the cdmsbats processing files.
The theoretical optimal filter resolution can be used to compare noise levels from each series. It can be calculated from the noise psd, J(f), and OF template, s(f), as
.
(Notes on discretizing this calculation and rectifying FT conventions can be found here)
We can now compare this resolution across the different data types and series. The calculated resolutions are again in the same units as PTOFamps. The mean resolutions for bkg, Na, and PuBe data were 8.79 nA, 14.6 nA, and 11.4 nA respectively.
Using these values, we can generate a list of the noisiest series. In PuBe data, the series with resolutions more than 3σ above the mean were:
//> 3-sigma 07180925_1410 07180927_2148 07180928_1913 07180929_0918 07181002_2002 07181003_0152
and those with resolutions 2σ above the mean were:
//> 2-sigma 07180923_0102 07180923_0436 07180923_0456 07180923_0617 07180923_1622 07180923_1905 07180925_0335 07180925_1410 07180927_1827 07180927_2148 07180927_2158 07180927_2208 07180927_2359 07180928_0030 07180928_0300 07180928_1913 07180928_2102 07180929_0559 07180929_0827 07180929_0918 07180929_1206 07180929_1445 07180930_0046 07181002_2002 07181003_0011 07181003_0152 07181003_0452 07181003_0741 07181003_0940
Noise Width from Randoms
A comparison was next made to the observed noise in each PuBe series. This was done by fitting the width of the PTOFamps0 distribution of randoms triggers in each series. The fitted widths are compared to the theoretical widths (as calculated above) in the figure below. There appears to only be a weak correlation between the two measures. There are some outliers in the measured quantity which are likely due to poor fits obtained form the automated fitting procedure. The rest of the poor agreement may be due to the selection of events which is used by the BatNoise algorithm to produce the PSDs used in the theoretical calculations.
At any rate, we can use these two measures to select series which are noisy according to both measures. This is defined as those series for which both measures of <m>\sigma_{PTOFamps}</m> are more than one standard deviation above the mean value for that measure. These are the series in red.
Effect of Noisy Series Cut
Spectra were produced using the full R68 data set, with all the standard cuts and both with and without these noisy series removed. The resulting spectra and passage fraction are shown below. There is no obvious structure uncovered in the (n,gamma) signal and the passage fraction is quite flat above the noise wall. So removing these series seems to just be an effective livetime cut with no clear improvement in signal. This is not surprising as the noise measures are generally stable to within 5%. For these reasons there seems to be no reason to apply a noisy series cut such as this in the final analysis.





