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2020/03/10 (Tuesday)

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Setup Run 72. DIB 1/3/4 → Stripline 43/41/48 → Cable 3/2/1 → nothing/nothing/accessory_interposer → HV_Conn 1/3/2 → HV 1/2 → DCRCX(4)/DCRC55(1). DCRCs on overnight. Lead/poly shield erected (4 lead walls, 2 poly walls).
Status Stopped circulation yesterday. Switched to one-shot, so we are pumping out of fridge and trap to dump. Suspend 1K Pot operation - 1K Pot is pumped out and isolated (maybe still has some LHe in it?)
0931 He recovery meter = 341037 cuft, rate 16 cuft/hour
1000 Tower/MC/Coldplate = 1.1/1.5/2.6 ± 0.1 K, Still = 21 ± 2 K / 0.022 mbar / 0.0 mW, G1/G2= 1.2/529.4 mbar, 1K Pot = >7K / 0.026 mbar. MB = -1%
1100 Turn off DAQ programs and power down DCRCs 1&4.
1115 Try measuring detector+electrode capacitance. Using the HP LCR meter. Leave DCRCs plugged in so that they connect all the Side1 channels to ground. Connect one meter lead to the shell of the HV input (Detector Side1 channels) and the other lead to the shell of the test resistor cable (to electrode).
1125 At low oscillation-level setting, capacitance reading was really low. Turn it up to something like 0.7 V, reading is more reasonable. Expecting something like 20 pF. But we are getting various values - sometimes around 30 pF, but as high as 170 pF, not very stable.
1130 Try various frequencies. “Q” is maximum (12.2) at 2 MHz. At this frequency C = 130 pF.
Freq [Hz] Q C [pF]
10e3 CF 70-100
20e3 CF 90-120
40e3 CF neg 300-500 (??)
100e3 -1.4 78-80
200e3 -2.4 84
400e3 -12.4 93.8
1e6 -2.71 82
2e6 -21.1 119.7
4e6 19.59 128.13
10e6 0.9 34
1200 Let's connect the HV side to Pin 1 at the cable, instead - this bypasses the 40 MOhm resistors. But this gives some nonsensical results.
1300 Set up to measure R and C using Wavetek Function Generator and oscilloscope, apply AC voltage at test resistor, measure Vinput and Vtest with scope.

Sine-wave measurement:

measurements:
freq Hz 11.67 3.347 0.334
I shift s -6.00E-03 -2.20E-02 -0.625
Vin V 9.68 9.68 9.68
Vtest V 0.24 0.216 0.068
calculations:
phase radians -0.439948635 -0.462656067 -1.311614933
omega Hz 73.32477253 21.02982122 2.098583893
RC s 0.02897268 0.095339259 0.126344816
I A 2.40E-07 2.16E-07 6.80E-08
C pF 793.9344846 2377.33359 3463.062931
R MOHm 36.49253279 40.10344151 36.48354606
  • In the above table RC constants are calculated from measuring V at two different times.
  • Vtest measured across 1 MOHm test resistor, gives the current
  • Expected R is 21 MOhm, this is the two 40 Ohm resistors to the HV in parallel

Square-wave measurement:

measurements:
with pi filters without pi filters
RC s 0.119223742 0.035690445
Vmax V 10 9.9
Vtestmax V 0.288 0.36
calculations:
I A 0.000000288 0.00000036
R MOHm 34.72222222 27.5
C pF 3433.643769 1297.834364
  • These function-generator measurements give huge capacitances.
  • Removing the pi filters definitely changes the result
1320 In the square-wave measurements there's also a very short initial fall, 300-400 us. Divided by 20 MOhm implies 20 pF. Well that's interesting…
For the fast time constant case: RC/Vin/Vtest = 0.4ms/9.9V/7.0V → R/C = 1.4 MOHm / 282 pF

OK, a muddled and confusing picture all around.

Note: none of the function-generator observations gives any indication of a polarity asymmetry. So nothing giving a clue to the polarity asymmetry in Luke gain.

1331 He recovery meter = 341100 cuft, rate 15 cuft/hour
1355 Open 1K Pot speedivalve to check pressure: about 0.2 bar on the mechanical gauge.
Pump out 1K Pot in steps with the 4He pump. Note that 1K Pot temperature does not fall. How warm is it? 1K Pot > 7K; Sorb = 10.2 K. So Pot is well above 4K but well below 77K.
1415 1K Pot is down to 0.5 mbar and flat. Stop pumping 1K Pot and isolate it again.
1425 G2 (dump) = 585 mbar and rising. G1 (condenser) = 0.9 mbar, slowly falling. P1 (still) = 0.020 mbar, slowly falling. Tower = 1.07 K, behaving as a 1K Pot as we continue in one-shot mode.
1430 Isolate fridge (close V1 and Still Gate valve) then open V3 to pump remains of cold LN2 Trap 1 directly to dump. Tower temperature starts to rise.
1435 IVC = 54 ubar. (We stopped pumping it yesterday, hasn't gone up much.)
1440 Isolate LN2 Trap 1 and remove it from the LN2 bath to warm up.
1440 Tower = 1.53 K and rising
1445 Close V6 to stop pumping mixture. Open fridge to GHS again. Then let mixture from dump into both sides of fridge through V4 & V3. Tower rises quickly to 3.7 K.
1450 Tower/MC(H35) = 3.5/3.4 K
1500 Let some He gas into the IVC, less than a tube-length. IVC → 40 ubar. Tower temperature rises quickly above 4K. Fridge pressure rises, G1 500→560 mbar.
1K Pot falls to 6.1 K, then rises again.
Isolate IVC then connect turbo pump manifold to cryostat vacuum jacket port
1500 Tower/MC(H35) = 5.0/5.0 K
1503 He recovery meter = 341123 cuft, rate = 15 cuft/hour
1515 Let 1.9 mbar He gas into vacuum manifold. Then open cryostat vacuum jacket valve to let this into the vacuum jacket. Vaccum Jacket → 0.046 mbar.
Recovery meter speeds up.
1524 He recovery meter = 341148 cuft, rate = 192 cuft/hour
1535 MC(Cernox) = 5.66 K and rising
1610 MC(Cernox) = 8.21 K and rising. G1 (fridge) = 584 mbar.
1615 Start pumping mixture from fridge (both sides) to dump.
1607 He recovery meter = 341230 cuft, rate = 90 cuft/hour
1630 MC(Cernox)/Sorb = 8.51/16.0 K and rising
1630 G2(dump) = 701.0 mbar, still rising slowly. (Around 701.7 before turning off the pump.) Fridge pressure has bottomed out. Stop pumping out fridge.
1717 He recovery meter = 341300 cuft, rate = 46 cuft/hour
1800 Around this time recovery meter starts moving a lot more slowly.
MC(Cernox) = 22 K

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