Ops Shift Transition: 06/20/2019, Owl Shift 07:00 – 15:00 (00:00-08:00) - UTC (PT)
State of H1: Locked
Intent Bit: Observing
Weather: 10-25 mph wind, cloudy
Primary 0.03 – 0.1Hz: 0.01 um/s
Secondary 0.1 – 0.3Hz: 0.1 um/s
Outgoing Operator: Jeff
Quick Summary: Locked and observing for half an hour. Wind has been high throughout the day, preventing lock, but according to Jeff it should be winding down.
Accepted the two ASC SDF Diffs listed below, in order to get back into Observing.
The IFO has been down for the first half of the shift. The high winds continue with base line speeds in the mid-20mph range. There are continual gusts into the mid to upper 30mph range. The forecast calls for the winds to subside later in the evening. The first half of the shift saw three earthquakes of mag 5 and larger. Went into EARTHQUAKE mode for the mag5.8 from Vanuatu. Was able to switch earthquake states while the IFO was locking without apparent problems. Will try running an initial alignment and relocking when the winds lay down a bit.
Georgia, Sheila, Patrick
Twice today we had locklosses for environmental reasons, and while Patrick was relocking we had the chance to try out the PRMI ASC. We fixed some bugs and the guardian path through PRMI ASC should now be working. It is still an optional path, so in ISC_LOCK if operators think that they would like to do PRMI they have the choice between the way things used to work (select PRMI_LOCKED, align by hand) and selecting PRMI_ASC, which will run the PRMI ASC (MICH and PRM loops), and wait for it to converge, and offload the ASC to the sliders. If you select nominal low noise the guardain will then move on to DRMI.
Laurence Datrier. Sheila Dwyer
A follow-up to alog 49682
We convolved our results for BNS range and duty cycle as a function of wind speed with wind speed frequency for O3 (data from 1st April 2019 to 2nd June 2019). We compare the average BNS range and duty cycle to the range if we were independent of the wind. In order to do this we approximated the DC and BNS range if wind-independent to wind values before there is a significant decay (usually 10th to 15th percentile). This is done for 1min max trends for the wind, and 30min max trends.
| Trend | Average BNS range (Mpc) | Average wind-independent BNS range (Mpc) | Improvement (Mpc) | % improvement on detection rates (based on volume) | Average duty cycle | Average wind-independent duty cycle |
| 1min max | 109.31 | 109.85 | 0.54 | 1.48% | 75.15% | 84.73% |
| 30min max | 109.31 | 110.23 | 0.93 | 2.50% | 75.61% | 83.66% |
FAMIS 10514 The level appears close to the max line, so I did not add any water. The bottom left canister is yellowed. There are no errors on the diode chiller.
TITLE: 06/19 Day Shift: 15:00-23:00 UTC (08:00-16:00 PST), all times posted in UTC STATE of H1: Lock Acquisition INCOMING OPERATOR: Jeff SHIFT SUMMARY: Second day of NSF review. Calibration measurements and noise budget. LOG: 15:15 UTC NSF reviewer through gate 15:17 UTC NSF reviewer through gate 15:21 UTC NSF reviewer through gate 15:21 UTC NSF reviewer through gate 15:27 UTC Karen leaving mid Y 15:47 UTC Peter to optics lab Jenne leading tour in control room 16:32 UTC Jenne leading tour out of control room 17:30 UTC Transitioned from WINDY to EARTH_QUAKE for 6.5 magnitude earthquake in Papua New Guinea Lock loss 17:35 UTC Peter back 17:49 UTC Georgia and Sheila testing PRMI 18:07 UTC Restarted video0 19:35 UTC SEI_CONF back to WINDY 20:05 UTC NLN 20:08 UTC Observing 20:08 UTC Sundae to optics lab 20:31 UTC Apollo through gate 20:34 UTC Running CAL measurements 21:10 UTC Peter to optics lab 21:25 UTC Done CAL measurements 21:37 UTC Georgia running noise budget 22:29 UTC Kyle to mid Y 22:36 UTC Lockloss
20:08 UTC Accepted attached ASC SDF differences.
Attached is an image showing two years worth of scroll pump tip seal (PTFE) wear accumulation in the scroll pump used to back our VBOD RGA turbo. Unlike our typical scroll pumps which experience viscous flow from time to time, either as the result of rough pumping a volume from atmosphere or from an introduced ballast purge, this pump has never experienced viscous throuput.
The "amount" of wear (dust) is normal and is a function of run time. Of interest here is the degree of accumulation and not the degree of generation.
Note that this dust would be "blown" out of the exhaust port if/when this pump were to pump a viscous load :)
We fix one problem and create another. Might be worth pumping air through the RGA scroll from time to time.
Tuesday afternoon I restarted the mx_stream process on h1susex (14:56 PDT) and h1seiex (14:57 PDT). Since that time we have had two h1seiex DAQ-CRC error events.
BTW: I'm detailing this problem on this wiki page
This is a continuation of the investigation in this aLOG comment: https://alog.ligo-wa.caltech.edu/aLOG/index.php?callRep=49620 I've plotted 48 hours of data beginning at 19:00 UTC on April 25, 2019. The goal was to capture the SR3 change noted here: https://alog.ligo-wa.caltech.edu/aLOG/index.php?callRep=48787. There is no obvious noteworthy change in the spring frequency or quality factor seen in this plot, only the usual changes in the few hours at the beginning of each lock stretch. The last plot shows trends of DeltaL / Pcal for the same 48-hour period, comparing C00 to a calibration that additionally corrects for time dependence in fs and Q, as well as kappa_PUM and kappa_UIM. It is consistent with the result of the previous aLOG comment, showing that compensating for more time dependence consistently improves calibration accuracy.
Quick trend comparing SRC spring freqnuency against BNS range and DRMI power levels. This will be done much more carefully ... soon.
[J. Kissel, A. Viets] At Jeff's request, I made time series plots of the SRC optical spring squared frequency with several front-end channels on the same plot, to see which are highly correlated. Additionally, I've listed (in the same order as the plots) the Pearson correlation coefficients between fs^2 and each other channel. Note that the correlation is reduced by two effects: first, fs^2 is not computed during lock loss and therefore remains constant, and second, noisy fluctuations (on ~2 minute time scales for fs^2, since that is about how much input data is used to compute each output value) are probably not correlated. Channel Name Name in Plot Correlation Coefficient Description H1:LSC-TR_Y_NORM_INMON TRY -0.07759334 arm cavity power, normalized to power when the Y arm is locked alone H1:LSC-TR_X_NORM_INMON TRX -0.07641386 arm cavity power, normalized to power when the X arm is locked alone H1:LSC-POPAIR_B_RF90_I_NORM_MON POP90 0.00209429 45 MHz sidebands inside PRC H1:LSC-POPAIR_B_RF18_I_NORM_MON POP18 0.05289885 9 MHz sidebands inside PRC H1:LSC-PR_GAIN_OUT16 PRG -0.0719822 power recycling gain H1:LSC-POP_A_LF_OUT16 POP DC -0.09153975 power inside the PRC H1:LSC-REFL_A_LP_NORM REFL DC 0.01795835 power reflected off of the input to PRM H1:IMC-MC2_TRANS_SUM_OUT16 IMC TRANS -0.08331603 power transmitted from the IMC By eye, the power recycling gain, the power in both arm cavities, the power in the PRC, seem to be consistently negatively correlated. So it would appear that the SRC's optical spring frequency is related in some way to the power circulating in the detector. Note the physical meaning of fs^2 as we have defined it: a positive value indicates an optical anti-spring, and a negative value indicates an optical spring. Based on these results, more power in the detector => optical spring is less "anti" and more "pro."
The original aLOG entry shows that correcting for time-dependent systematic errors in the sensing function assuming a model with SRC detuning improves calibration accuracy at the lowest Pcal line frequency. Given that we now believe the primary cause of low-frequency time-dependent systematic errors in the sensing function is a parasitic coupling of angular motion sensing to DARM rather than SRC detuning (see G1901353 and LHO aLOG 50992), I wanted to investigate whether correcting for SRC detuning could lead to an overall improvement in calibration accuracy. The short answer is "Well, close to the lowest Pcal line, yes, but not reliably at other frequencies." I used four Y-end Pcal broadband injections (RX channel), and plotted DeltaL / Pcal from 10-400 Hz for two calibrated data sets: one that corrected for all modeled time-dependence except SRC detuning (spring frequency f_s and quality factor Q), and one that additionally includes time-dependent corrections for SRC detuning. In order to get a measurement of all time-dependent correction factors, I started the gstlal calibration pipeline ~1 hour before the broadband injection, since the calibration lines are turned off during the injections. The dates and associated aLOGs are listed below in the same order as the plots:
Text files with the data of the plots in the previous comment can be found in the calibration SVN in this directory:
aligocalibration/trunk/Runs/O3/H1/Measurements/FullIFOSensingTFs/
with names like
H1_With_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_[GPS_START_TIME]-[DURATION].txt
for data corrected for "SRC detuning" time dependence and names like
H1_Without_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_[GPS_START_TIME]-[DURATION].txt
for data that is not.
Since there is now precedent, I've moved and committed the above mentions "DCS analysis of broadband injections" text files in to the DCS_BB_plots/ directory, e.g.
/ligo/svncommon/CalSVN/aligocalibration/trunk/Runs/O3/H1/Measurements/FullIFOSensingTFs/DCS_BB_plots/
H1_Without_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1244406526-120.txt
H1_Without_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1246226240-120.txt
H1_Without_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1247431237-120.txt
H1_Without_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1248718240-120.txt
H1_With_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1244406526-120.txt
H1_With_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1246226240-120.txt
H1_With_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1247431237-120.txt
H1_With_SRC_Corrections_over_CAL-PCALY_RX_PD_OUT_DQ_1248718240-120.txt
TITLE: 06/19 Day Shift: 15:00-23:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Observing at 113Mpc
OUTGOING OPERATOR: TJ
CURRENT ENVIRONMENT:
Wind: 21mph Gusts, 16mph 5min avg
Primary useism: 0.07 μm/s
Secondary useism: 0.08 μm/s
QUICK SUMMARY:
No immediate issues.
TITLE: 06/19 Owl Shift: 07:00-15:00 UTC (00:00-08:00 PST), all times posted in UTC
STATE of H1: Observing at 116Mpc
INCOMING OPERATOR: Patrick
SHIFT SUMMARY: Normal recovery after the earthquake rang down, and then we have been locked for 4.5hrs since.
LOG:
Winds have picked back up to 30mph. 1.5hour lock. We dropped Observing briefly due to the squeezer losing lock, but it relocked quickly.
After the EQ calmed down, I ran an initial alignment and then it relocked. Accepted a few ASC and LSC SDFs.
Contractor spent the day installing new components on all eight liquid nitrogen Dewar fill lines to bring skids up to industry standard. Components include check valve, pressure relief valve, strainer, and drain valve. At their recommendation, a support stand was installed and anchored into concrete upon hammer drilling holes. Corner and end station skids were completed before noon to minimize impact on observing.
Check valve = Nibco class 200 bronze T-453-B 1.5"
Drain valve = Rego Goddard T9454 1/2" F.NPT with BK9450R stem
Strainer = Mueller Steam Specialty LF352 1.5" with non-standard 100 mesh for cryogenic application
Pressure relief valve = rated for 350 psi
Picture of CP1 skid attached.
Note: the existing pressure relief valve just upstream of the control module safety valve on all skids, except CP1 skid, was removed to accommodate stack up length of new components
Worth noting that contractor purged pipe with gas N2 while brazing to prevent scaling on the inner surface.
The new strainer mesh is intended to prevent debris from entering the system, but does not filter ice. Contractor recommends cleaning it 2x/yr.