UMN CDMS Wiki archive
start › cdms › k100 › run_summary › run_75

Run 75 Summary

Run preparation

Setup

Run 75 Channel Map
Tower Cable DCRC(2sided) Label HV output, Side1-readout HV output, Side2-readout
Face5pA Cable 2 (includes LEDs)
HV CONN1
DCRC1 Side1pE HV1 pA -
Face5pB Side1pB HV1 pB -
Face5pC Side1pD HV1 pC -
Face5pD Side2pE - HV2 pD
Face3pA Cable 1 (includes accessories)
HV CONN2
DCRC3 Side2pC - HV2 pA
Face3pB Side2pF - HV2 pB
Face3pC Side1pC HV2 pC -
Face3pD Side1pF HV2 pD -
Face2pA Cable 3
HV CONN3
DCRC4 Side2pB - HV1 pA
Face2pB Side2pA - HV1 pB
Face2pC Side1pA HV2 pB -
Face2pD Side2pD - HV1 pD

IbIs measurements

Overview of automated IbIs technique

This plot compares the TES resistance (normalized to R_normal) to dP/dI. I've been setting
the QET biases to match dP/dI = 1.0 μV. This is pretty different from fixing a certain
fraction of Rn. The resistance fraction is pretty high for some of the Side2 channels.

TES properties

Channel Tc [mK] Rn [mΩ] Rpar [mΩ] Rop/Rn
Side1pA 81.9 124.9 12.1 0.42
Side1pB 86.0 95.0 15.2 0.58
Side1pC 77.0 73.4 8.3 0.63
Side1pD 78.0 89.7 13.1 0.50
Side1pE 76.0 89.1 10.7 0.52
Side1pF
Side2pA 72.5 68.6 6.8 0.61
Side2pB 77.5 65.6 7.6 0.60
Side2pC 70.0 60.8 11.0 0.79
Side2pD 69.9 76.3 12.2 0.62
Side2pE 69.0 69.9 15.1 0.79
Side2pF 69.0 58.7 9.2 0.83
Average 75.2 79.3 11.0 0.63

Notes:

  • Critical temperature (Tc) is an average of all measurements. In some cases the start and end temperatures were measured while warming and cooling; in others only one value was measured while cooling.
  • Resistance measurements are based on the assumption that Rshunt = 8.0 mΩ.
  • Normal resistance (Rn) shown are from IbIs taken around 42 mK. From the earlier IbIs taken at 50-56 mK the Rn's come out around 5% higher on average.
  • Parasitic resistance (Rpar) is based on fitting the lowest part of the transition curve (not sure about the accuracy).
  • Operating resistance as a fraction of normal (Rop/Rn) is based on the standard adopted for Run 75 (at least for 2-sided 0-V data) of choosing a point in transition at which dP/dI = 1.0 μV. Figures shown are for temperatures around 42 mK which is the average base after the early part of the run. But they're not much different at higher temperatures.

Source mover

Source mover is mounted above Side 1 and the far endstop is oriented in the +y direction. The +y direction is toward pC, away from pD on both sides, and “parallel” to pE.

Position studies

Noise width

As of 2022 Feb 7 the best noise width measured is 6.5 eVee, for Side1 with pF not working, at approx +100V bias with pre-biasing and with the source situated at y=30mm, above pC.

The following plots illustrate how this was measured:

07220205_1128: Side1 readout, 98.1V with 5min/15% prebias, Source y=30.03mm
Cut to select lower Am-241 peaks. Note INT quantities are used instead of OF
Comparing OF to INT shows saturation effects in fitting, OF flattens out by 60keV. Clearly PT pulse shape is much different even at the lower Am peaks.
Here we plot INT versus OF to “linearize” OF (with respect to INT). The fit is a quadratic fixed at (0,0) and extending out to the 14keV peak
Low-energy Am spectrum using “linearized” OF. Use the 14 keV peak to calibrate to keVee.
Standard noise-width plot: calibrated&linearized OF plotted for 1000 randoms using OF0 quantity (fixed-time OF fit)
07220213_2057: Side2 readout, 98.6V with 5min/15% prebias, Source y=0.03mm
For some reason with Side2 data, the peaks are more difficult to see in either OF or INT.
This can be seen in this plot: projecting the peaks to either axis you get a lot of overlap,
although the peaks are relatively well resolved along diagonal lines - which means that
the ratio of OF to INT has better energy resolution - which means pulse shape has
better energy information around 14keV than amplitude.
Here we see how strongly pulse shape changes with amplitude. PT pulse width (40% rise to 40% fall) versus PT_integral is plotted.
Same as above with low Am-peaks highlighted
Turns out PT width produces rather good energy peaks. I've used these to select 14 keV peaks to calibrate PTOF (after linearizing).

The table below summarizes the noise widths measured during this run under various conditions:

Readout Source position Bias [V] Bias polarity Prebias dP/dI [uV] Noise width [eVee]
2-sided pF 0 n/a n/a 1.0 130
side1 pF 20 + no 1.0 18.7
side1 pF 100 + no 1.0 11.8
side1 pF 150 + no 1.0 16.9
side1 pF 100 + yes 1.0 8.1
side1 pC 100 + yes 1.0 6.5
side1 pC 100 - yes 1.0 7.3
side2 pC 100 + yes 1.0 5.18
side2 pF 100 + yes 1.0 8.1
side2 pF 100 + yes 0.9 5.53
side2 pF 100 + yes 0.7 4.7
side2 pF 100 + yes 0.4 8.56

Some observations:

  • 100V seems to be better than 150V, though this is not certain (comparison only without prebias)
  • There seems to be a sweet spot for dP/dI. The lowest value (highest gain) has worse noise width. Possibly because electrothermal oscillations get worse.

The same noise-width calculation technique was performed on background data from Run68 using S101. This is for the conditions that we decided were optimal. Results below:

S101 noise width from Run68
Readout Source position Bias [V] Bias polarity Prebias dP/dI [uV] Noise width [eVee]
side1 pF 125 - yes vary with channel, 0.5-1.0 8.3

Interestingly the Run68 data shows much less pulse-widening in the 0-20 keVee range. Why is this? Tc's and Rn's are about the same.

S104, this run, 100V S101, Run 68, 125V

Tower Thermometer versus Goldman Thermometer

As in previous runs the Tower Thermometer (connected to the fridge wiring) read anomalously high. The Goldman thermometer (connected to stripline wires) seemed to read correctly. The spreadsheet below compares the two thermometer readings taken at the same time once a day.

temerpature_comparisons.xlsx