Following our influx of bees, M. Landry ordered an interior inspection of each beam tube enclosure (BTE) interior to document potential areas of ingress. R. Thompson with Apollo Mech is presently tasked with this inspection. During inspection of the X1 enclosure, roughly 5 sections -X of the X arm overpass, Randy observed cracking at the base of the interior of the enclosure. After further investigation he found 4-5 cracks running parallel of one another across the entire section at roughly the 10 & 2 o'clock positions. I was called to come give this section a second look. The cracks were also immediately concerning to me. The first thing I wanted to better understand was the interior width to assess if the section was shifting. With Randy's help, I measured the interior spans of each end of the neighboring tube sections (4 measurements) as well as an additional 4 of the same spans of the tube sections on display outside of the LExC. On average, these spans measure 151" +/- .25". The section in question measures 154" at each end. Moreover, during installation Fred Raab has informed us that grouting was done on the BTE interiors to mitigate a "walking" effect that was causing misalignment between sections. This grouting has clearly separated from the BTE interior which confirms that there is in fact splaying of this section. The current short term "fix" implemented by FAC and VAC has been the erection of scaffolding topped with planking across the 10' area of beam tube at risk of falling debris. This should act as makeshift roof. For the long term, R. McCarthy is currently consulting with structural engineers whom we hope can help us work up a solution to prevent further splaying. Contained in the photos attached are measurements with appropriate labeling of each section (number counted from second door on X1 traveling -X), as well as a "+X" or "-X" which simply denotes if the measurement is on the +X or -X end of the tube section, photos illustrating the separation of the BTE interior from the as-installed BTE grouting, the scaffolding presently in place, the cracking at the footing/mid sections, and a LIGO Yelp review written in welders soapstone (circa ~96') near the splayed tube section. C. Soike, E. Otterman, T. Guidry, G. Moreno, T. Sadecki, J. Vanosky, R. McCarthy
J. Kissel, M. Pirello There are four pico-motor actuated mirrors in the HAM2-3 ISI SPI Pathfinder (or, generically HAM2 = ISI"J" and HAM3= ISI"K"), M_M1, M_C1, M_B4, and M_M2 (see page 3 of D2400108). Those optics have the following mounts: - M_M1 = IXM100.C2L-VC LIGO = 1" optic mount, left-handed. - M_C1 = IXM200.C2-VC LIGO = 2" optic mount, right-handed. - M_B4 = IXM100.C2-VC LIGO = 1" optic mount, right-handed. - M_M2 = IXM100.C2-VC LIGO = 1" optic mount, right-handed. To-date the assembly procedure has been scattered into incomplete pieces, including separated mechanical assembly (D1100362 and E2500163-v1) and electrical assembly (D1400279). As such, I've created an all-inclusive assembly procedure in E2500163-v2, and the DCC file-card now perma-links to a google photo album containing many more photos than even what's in the procedure. So, now I can write this aLOG, which "just" says -- we've completed the assembly for SPI's four pico-actuated mirrors, per E2500163-v2 assembly instructions. It's always challenging to get a photo highlight, so I'll attach the best one I got mid assembly (i.e. the picomotors weren't yet connectorized, nor were the ECR E1400327 range-limiting shafter collars installed). The 2nd, 3rd, and 4th attachment show three photos I got of the completed M_M1 (IXM100.C2L, 1" left-handed) mount.
Jenne allowed us to quickly drop from observing to change the EY camera offsets. Yesterday we updated them 87473 but didn't load the camera servo guardian, so the guardian did not use the correct lscparams file. This meant that the A2L gains (ISC_LOCK controlled) were set for the new spot, but the camera offsets (camera servo guardian controlled) were at the old spot. This was also missed because these values are not monitored in the observe SDF files. We noticed that:
Many of these are issues are documented in Ryan's shift alog here: 87485.
We dropped out of observing and I set the EY camera offsets to their proper value. This immediately began increasing the PRG and arm power. Then, I loaded the camera servo guardian so that when we relock these values are set properly. Then, I proceeded to monitor all the camera offsets and A2L gains and accept their new values in OBSERVE. This will cause SDF differences if these values change. However, I think these are important enough settings that we should be monitoring them for observing.
Kappa C has increased and the calibration monitoring lines are now back to 2% or less.
TITLE: 10/15 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Observing at 150Mpc
OUTGOING OPERATOR: Ibrahim
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 0mph Gusts, 0mph 3min avg
Primary useism: 0.08 μm/s
Secondary useism: 0.13 μm/s
QUICK SUMMARY:
It looks like the same PI that rung up yesterday and almost caused a lockloss is still ringing up, although not as strongly. This suggests, along with other evidence, that we are still not at the right beam position on ETMY. This is on the to-do list to investigate tomorrow, and hopefully we will stop ringing up this PI. See 87473.
The circulating power looks lower than the previous weeks locks, kappa_c also looks lower this lock.
Ryan's data above in consistent with what we saw yesterday too. This makes me think that we should readjust the spot before running the calibration measurement tomorrow.
I ran the range comparison against a lock last week with better range, lot of extra low frequency noise.
We did not load the camera servo guardian yesterday after the changes, so the new camera offsets did not get properly loaded and engaged when the camera servos came on. We are back at the old camera offsets for ETMY, but at new A2L gains based on where we set the camera offsets yesterday. So, the buildups are bad because we're at the wrong beamspot on EY, and the sensitivity is bad because the beam spot is not lined up with the mirror actuation point, so we have extra ASC coupling, as Ryan's plot above shows.
Neither the A2L gains nor the camera offsets are monitored in SDF, so this was not caught until just now.
Calibration monitoring line at 33 Hz was also 1% worse than yesterday.
Wed Oct 15 10:05:11 2025 INFO: Fill completed in 5min 8secs
Gerardo confirmed a good fill curbside.
The chilled water plants at the Mid stations have been shut down for the Winter.
TITLE: 10/15 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Observing at 156Mpc
INCOMING OPERATOR: Ibrahim
SHIFT SUMMARY: Observing at 155 Mpc and have been Locked for about 8.5 hours. Nothing happened during my shift besides a couple of ITMX saturations.
LOG:
23:00UTC Observing and Locked for almost 3 hours
23:34 Left Observing to close beam diverter
23:34 Back into Observing
Still Observing and have been Locked for almost 7 hours. Secondary microseism has continued to drop. Our range has been a bit better than it has been the last couple of days, so that's cool.
First attachment is a screenshot of D1300130 ISS array PD assembly (which is somehow called "PSL PDD MODULE").
Each PD (part #8) is entirely retained in an aluminum cylinder called the PDD main photodiode mount (part #9) and therefore the can of the PD is conductive to the cylinder. However, the cylinder is supposed to be isolated from the ISS array plate (and therefore the entire ISS array structure) by two pieces of kapton insulators (part #10). PCB assembly, which is connected to the PD, is sandwiched between two aluminum clamps (part #2 "PDD clamp" and part #11 "Clamping plate", which I refer to the bottom and the top clamp respectively), but the PCB ground is isolated from the clamps by an insulator ring (part "7?").
This way ground loop is broken even though the can of the PD is connected to the shield of two SMP coax cables on the PCB board (part #1).
Rahul and I checked the continuity between the cylinder and the ISS array cage. (Note that this check could not be done without disconnecting all SMP cables from the preamp first, because the preamp's ground is somehow connected to the optics table, which is connected to the ISS array cage.)
Issues found on the installation spare:
Unfortunately two of the PDs on the first floor (PD 5 and 6 in our notation in the lab, see the 2nd picture for the notation even though that is the picture of the 3IFO unit) didn't pass the check.
We also checked the grounding of the QPD and it was good.
Inspecting 3IFO, finding the same issue, and fixing it:
We quickly checked the 3IFO unit too and found that it also had a grounding issue for one of the PDs (PD 2). In the 2nd attachment, you can see that the space between the top and the bottom clamp of PD2 is smaller than the others.
We removed the top clamp and found no insulator (3rd attachment). We disconnected the PCB from the PD and learned that:
Fixing the issue on the installation spare:
With the new knowledge about the insulator, we looked at the gap between the top and the bottom clamps of the PDs for the installation spare unit and it looked like PD5, 6, 7 had the insulator on the wrong side of the PCB even though PD7 didn't have the grounding issue.
Sure enough, we removed the top clamp for these problematic PDs, found no insulator for any of these (5th attachment), removed the PCB and found the insulator on the wrong side (6th attachment shows you one example), installed them correctly and the grounding problem was gone.
Electrical test:
Since we have disconnected the PCB and reconnected to the PDs, we reconnected all of the PDs to the preamp again and confirmed that all PDs still respond to the light as they used to.
We haven't measured if any one of these are much noisier than the others, which we'll check later.
Closes FAMIS#28427, last checked 87380
ITMX had too low of coherence again this week so it didn't run. Everyone else is looking normal.
Jennie W, Keita, Rahul
On Friday, Keita and Rahul and I tried moving PDs 2 and 6 to align them better with the others. As can be seen from the scans we did of the DC voltage of the diodes as we moved the input alignemnt in horizontal translation and yaw from alog #87290, 2 and 6 have a range of alignment that is shifted relative to the other 6.
We also checked this with a IR sensitive camera with a zoom lens.
One person used the camera with a zoom lens to check the spot on the PDs as another person loosened the screws from behind the array and the third person held the barrel of the PD assembly to stop it moving or rotating in an undesired direction.
There is not a lot of space as 2 and 6 are in a column and are very close to diodes 1 and 5 on the right.
The horizontal scan we took after these moves showed we had made things worse, see this image.
Later that afternoon, Keita moved the PD 2 back and checked the alignment and it looks better.
The alignment as of yesterday (Monday) was 143mm in pitch (as read out by the allen key in the PZT mirror pitch actuator wheel) and 0.4145 inches in horizontal translation as read out by the translation stage the PZT mirror sits on.
Keita measured the coupling (after finding an error in my code from the previous coupling measurement I plotted last Thursday (alog #87400)).
The coupling in both vertical and horizontal is below 10, so this should be good enough for install if all else checks out.
Yesterday afternoon, Rahul and I did the vertical scan (slightly off from the horizontal reference position of 0.4145 inches that Keita had aligned to). The data in this graph was collected at a horizontal translation stage reading of 0.4162 inches.
We had to redo the horizontal scan today as I missed out some scan values yesterday. The data was collected with the pitch indicator at 143mm (the allen key on the pitch wheel actuator).
This morning Rahul recentred the QPD on the input beam (translation stage = 0.4145 inches, allen key - 143mm) and we scanned the translation stage horizontally to measure the calibration of the QPD.
This first scan had too large steps to give a good estimate of the slope for the X coordinate on the QPD near the centre, so I repeated the measurement with smaller steps. Although I thought I set the laser to ~120 mA for both measurements the power on the QPD sum was slightly different between the two, see this plot where the original measurement set is in orange and the second set in blue.
Looking at the plot the QPD has the same slope in Y for both measurements but the second set of Y measurements has lower voltages.
The X data overlaps between the two measurements which makes more sense to me, as we assume the QPD electronics normalise the readout of X and Y by the sum channel to account for power fluctuations.
I used the newer measurement to estimate the calibration in the x direction, and the older measurement to estimate the slope in the y-direction, I tried to only use the linear part of the data in my fit and also not use any points with a voltage abive 6 Volts as this is when we expect the QPD to not be linear.
The calibration plot is here with the X calibration line in orange and the Y calibration line in red.
The resultant calibration is 72.0 V/mm in the horizontal direction, at an angle of 7.4 deg with the QPD axis. This is similar to the last calibration we did before several moves of the QPD to recentre it, see alog #87375.
This is worked out by adding the two slopes in quadrature and using atan2(Y_calib/X_calib) to work out the angle of the QPD axis with the horizontal direction of the PZT mirror translation.
Attaching a picture of the recentered QPD on the input beam.
WP 12836
ECR E2400330
Modified List T2500232
The following SUS SAT Amps were upgraded per ECR E2400330. Modification improves the whitening stage to reduce ADC noise from 0.05 to 10 Hz.
Suspension | Old | New | OSEM |
ETMX L2 (PUM) | S1100146 | S1100119 | ULLLURLR |
ETMY L2 (PUM) | S1100137 | S1100127 | ULLLURLR |
ITMX L2 (PUM) | S1100135 | S1100118 | ULLLURLR |
ITMY L2 (PUM) | S1000277 | S1100148 | ULLLURLR |
F. Clara, J. Kissel, O. Patane
Here's the characterization data and fit results for S1100148, assigned to ITMY L2's ULLLURLR OSEMs.
This sat amp is a UK 4CH sat amp, D0900900 / D0901284. The data was taken per methods described in T080062-v3, using the diagrammatic setup shown on PAGE 1 of the Measurement Diagrams from LHO:86807.
The data was processed and fit using ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Scripts/
plotresponse_S1100148_ITMY_L2_ULLLURLR_20250917.m
Explicitly, the fit to the whitening stage zero and pole, the transimpedance feedback resistor, and foton design string are:
Optic | Stage | Serial_Number | Channel_Number | OSEM_Name | Zero_Pole_Hz | R_TIA_kOhm | Foton_Design |
---|---|---|---|---|---|---|---|
ITMY | L2 | S1100148 | CH1 | UL | 0.095:5.19 | 120.5 | zpk([5.19],[0.095],1,"n") |
CH2 | LL | 0.0957:5.24 | 120.0 | zpk([5.24],[0.0957],1,"n") | |||
CH3 | UR | 0.0958:5.24 | 120.125 | zpk([5.24],[0.0958],1,"n") | |||
CH4 | LR | 0.0967:5.28 | 120.375 | zpk([5.28],[0.0967],1,"n") |
The attached plot and machine readable .txt file version of the above table are also found in ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Results/
2025-09-17_UKSatAmp_S1100148_D0901284-v5_fitresults.txt
Per usual, R_TIA_kOhm is not used in the compensation filter -- but after ruling out an adjustment in the zero frequency (by zeroing the phase residual at the lowest few frequency points), Jeff nudged the transimpedance a bit to get the magnitude scale within the ~0.25%, shown in the attached results. Any scaling like this will be accounted for instead with the absolute calibration step, i.e. Side Quest 4 from G2501621, a la what was done for PR3 and SR3 top masses in LHO:86222 and LHO:84531 respectively.
Here's the characterization data and fit results for S1100119, assigned to ETMX L2's ULLLURLR OSEMs.
This sat amp is a UK 4CH sat amp, D0900900 / D0901284. The data was taken per methods described in T080062-v3, using the diagrammatic setup shown on PAGE 1 of the Measurement Diagrams from LHO:86807.
The data was processed and fit using ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Scripts/
plotresponse_S1100119_ETMX_L2_ULLLURLR_20250916.m
Explicitly, the fit to the whitening stage zero and pole, the transimpedance feedback resistor, and foton design string are:
Optic | Stage | Serial_Number | Channel_Number | OSEM_Name | Zero_Pole_Hz | R_TIA_kOhm | Foton_Design |
---|---|---|---|---|---|---|---|
ETMX | L2 | S1100119 | CH1 | UL | 0.0949:5.19 | 120 | zpk([5.19],[0.0949],1,"n") |
CH2 | LL | 0.0971:5.32 | 120 | zpk([5.32],[0.0971],1,"n") | |||
CH3 | UR | 0.0964:5.27 | 120 | zpk([5.27],[0.0964],1,"n") | |||
CH4 | LR | 0.0957:5.23 | 120 | zpk([5.23],[0.0957],1,"n") |
The attached plot and machine readable .txt file version of the above table are also found in ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Results/
2025-09-16_UKSatAmp_S1100119_D0901284-v5_fitresults.txt
Per usual, R_TIA_kOhm is not used in the compensation filter -- but after ruling out an adjustment in the zero frequency (by zeroing the phase residual at the lowest few frequency points), Jeff nudged the transimpedance a bit to get the magnitude scale within the ~0.25%, shown in the attached results. Any scaling like this will be accounted for instead with the absolute calibration step, i.e. Side Quest 4 from G2501621, a la what was done for PR3 and SR3 top masses in LHO:86222 and LHO:84531 respectively.
Here's the characterization data and fit results for S1100118, assigned to ITMX L2's ULLLURLR OSEMs.
This sat amp is a UK 4CH sat amp, D0900900 / D0901284. The data was taken per methods described in T080062-v3, using the diagrammatic setup shown on PAGE 1 of the Measurement Diagrams from LHO:86807.
The data was processed and fit using ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Scripts/
plotresponse_S1100118_ITMX_L2_ULLLURLR_20250916.m
Explicitly, the fit to the whitening stage zero and pole, the transimpedance feedback resistor, and foton design string are:
Optic | Stage | Serial_Number | Channel_Number | OSEM_Name | Zero_Pole_Hz | R_TIA_kOhm | Foton_Design |
---|---|---|---|---|---|---|---|
ITMX | L2 | S1100118 | CH1 | UL | 0.0966:5.27 | 120 | zpk([5.27],[0.0966],1,"n") |
CH2 | LL | 0.0961:5.25 | 120 | zpk([5.25],[0.0961],1,"n") | |||
CH3 | UR | 0.0963:5.26 | 120 | zpk([5.26],[0.0963],1,"n") | |||
CH4 | LR | 0.097:5.3 | 120 | zpk([5.3],[0.097],1,"n") |
The attached plot and machine readable .txt file version of the above table are also found in ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Results/
2025-10-14_UKSatAmp_S1100118_D0901284-v5_fitresults.txt
Per usual, R_TIA_kOhm is not used in the compensation filter -- but after ruling out an adjustment in the zero frequency (by zeroing the phase residual at the lowest few frequency points), Jeff nudged the transimpedance a bit to get the magnitude scale within the ~0.25%, shown in the attached results. Any scaling like this will be accounted for instead with the absolute calibration step, i.e. Side Quest 4 from G2501621, a la what was done for PR3 and SR3 top masses in LHO:86222 and LHO:84531 respectively.
Here's the characterization data and fit results for S1100127, assigned to ETMY L2's ULLLURLR OSEMs.
This sat amp is a UK 4CH sat amp, D0900900 / D0901284. The data was taken per methods described in T080062-v3, using the diagrammatic setup shown on PAGE 1 of the Measurement Diagrams from LHO:86807.
The data was processed and fit using ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Scripts/
plotresponse_S1100127_ETMY_L2_ULLLURLR_20250916.m
Explicitly, the fit to the whitening stage zero and pole, the transimpedance feedback resistor, and foton design string are:
Optic | Stage | Serial_Number | Channel_Number | OSEM_Name | Zero_Pole_Hz | R_TIA_kOhm | Foton_Design |
---|---|---|---|---|---|---|---|
ETMY | L2 | S1100127 | CH1 | UL | 0.0963:5.26 | 121.25 | zpk([5.26],[0.0963],1,"n") |
CH2 | LL | 0.0958:5.24 | 121.25 | zpk([5.24],[0.0958],1,"n") | |||
CH3 | UR | 0.0952:5.2 | 121.25 | zpk([5.2],[0.0952],1,"n") | |||
CH4 | LR | 0.0954:5.21 | 121.25 | zpk([5.21],[0.0954],1,"n") |
The attached plot and machine readable .txt file version of the above table are also found in ${SusSVN}/trunk/electronicstesting/lho_electronics_testing/satamp/ECR_E2400330/Results/
2025-09-16_UKSatAmp_S1100127_D0901284-v5_fitresults.txt
Per usual, R_TIA_kOhm is not used in the compensation filter -- but after ruling out an adjustment in the zero frequency (by zeroing the phase residual at the lowest few frequency points), Jeff nudged the transimpedance a bit to get the magnitude scale within the ~0.25%, shown in the attached results. Any scaling like this will be accounted for instead with the absolute calibration step, i.e. Side Quest 4 from G2501621, a la what was done for PR3 and SR3 top masses in LHO:86222 and LHO:84531 respectively.