Thu Aug 07 10:07:03 2025 INFO: Fill completed in 6min 59secs
Lockloss at 2025-08-07 16:15UTC after 5.5 hours Locked due to some fast tractoring it's looking like an ETMX glitch :(
Ran our usual calibration measurements this morning following the wiki instructions. We plan to make some bias changes and then run this again. I'll comment to this log with that info.
Simulines start:
PDT: 2025-08-07 08:36:03.467961 PDT
UTC: 2025-08-07 15:36:03.467961 UTC
GPS: 1438616181.467961
Simulines end:
PDT: 2025-08-07 08:59:22.221768 PDT
UTC: 2025-08-07 15:59:22.221768 UTC
GPS: 1438617580.221768
Files:
2025-08-07 15:59:22,060 | INFO | File written out to: /ligo/groups/cal/H1/measurements/DARMOLG_SS/DARMOLG_SS_
20250807T153604Z.hdf5
2025-08-07 15:59:22,068 | INFO | File written out to: /ligo/groups/cal/H1/measurements/PCALY2DARM_SS/PCALY2DA
RM_SS_20250807T153604Z.hdf5
2025-08-07 15:59:22,072 | INFO | File written out to: /ligo/groups/cal/H1/measurements/SUSETMX_L1_SS/SUSETMX_
L1_SS_20250807T153604Z.hdf5
2025-08-07 15:59:22,077 | INFO | File written out to: /ligo/groups/cal/H1/measurements/SUSETMX_L2_SS/SUSETMX_
L2_SS_20250807T153604Z.hdf5
2025-08-07 15:59:22,081 | INFO | File written out to: /ligo/groups/cal/H1/measurements/SUSETMX_L3_SS/SUSETMX_
L3_SS_20250807T153604Z.hdf5
The lock loss that we had over night was unfortunately an ETMX glitch. We hadn't seen one since changing the ETMX bias July 28th so we were hopeful that it was the fix. Sad.
TITLE: 08/07 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Observing at 144Mpc
OUTGOING OPERATOR: Ryan C
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 5mph Gusts, 1mph 3min avg
Primary useism: 0.01 μm/s
Secondary useism: 0.08 μm/s
QUICK SUMMARY: Locked for almost 4 hours. Had a GRB (E587865) short come through at 1046UTC just a few minutes after we got to observing. Plan for today is commissioning and calibration from 1530-1900UTC.
TITLE: 08/07 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Observing at 151Mpc
INCOMING OPERATOR: Ryan C
SHIFT SUMMARY:
IFO is in NLN and OBSERVING since Aug 5 22:22 UTC (30 hr 40 min lock!)
Nothing to add other than well done everyone (particularly comissioners) for contributing to such a stable IFO state - this is definitely the O4c record so far.
LOG:
None
Ivey,
I finished the yaw-to-yaw transfer functions for the OSEM estimator using the corrected measurements that Oli took for SR3 yesterday [see LHO: 86202].
The fits were added to the Sus SVN and live inside '~/SusSVN/sus/trunk/HLTS/Common/FilterDesign/Estimator/fits_H1SR3_2025-08-05.mat'. They are already calibrated to work on the filter banks for the estimator and can be installed using 'make_SR3_yaw_model.m', which is in the same folder.
Attached below are two images of the fits for the estimator.
The first attachment shows the Suspoint Y to M1 DAMP Y fit. The zpk for this fit is
'zpk([0,0,-0.027+20.489i,-0.064+11.458i,-0.027-20.489i,-0.064-11.458i],[-0.072+6.395i,-0.072-6.395i,-0.096+14.454i,-0.096-14.454i,-0.062+21.267i,-0.062-21.267i],-0.001)'
The first attachment shows the Suspoint Y to M1 DAMP Y fit. The zpk for this fit is
'zpk([-0.002+19.224i,-0.007+8.31i,-0.002-19.224i,-0.007-8.31i],[-0.06+6.398i,-0.06-6.398i,-0.091+14.439i,-0.091-14.439i,-0.074+21.29i,-0.074-21.29i],12.184)'
TITLE: 08/06 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Observing at 147Mpc
INCOMING OPERATOR: Ibrahim
SHIFT SUMMARY: Very quiet day with H1 observing throughout except for just a few minutes this morning. H1 has now been locked for over 25 hours.
LOG:
| Start Time | System | Name | Location | Lazer_Haz | Task | Time End |
|---|---|---|---|---|---|---|
| 19:33 | SAF | Laser HAZARD | LVEA | YES | LVEA is Laser HAZARD | Ongoing |
| 15:43 | CAL | Rick | PCal Lab | Local | SPI BS measurements | 17:11 |
| 15:43 | FAC | Kim | Optics Lab | N | Technical cleaning | 16:14 |
| 16:19 | CAL | Dripta | PCal Lab | Local | SPI BS measurements | 17:11 |
| 17:52 | FAC | Randy | MY | N | Looking for materials | 18:22 |
| 18:34 | SPI | Jeff | Optics Lab | N | SPI measurements | 19:56 |
| 19:57 | VAC | Travis | MX | N | Leak checking | 20:30 |
| 20:53 | CDS | Marc | MY | N | Looking for parts | 21:31 |
| 21:14 | VAC | Travis, Janos | MX | N | Pump checks | 21:20 |
| 21:20 | ISC | Camilla | Optics Lab | N | Sorting totes | 22:38 |
| 21:44 | SPI | Jeff | Optics Lab | Local | SPI measurements | 23:11 |
| 21:54 | ISC | Jennie | Optics Lab | Local | ISS array work | 22:50 |
| 22:21 | CAL | Dripta | PCal Lab | Local | SPI BS measurements | 22:38 |
| 23:07 | ISC | Jennie | Optics Lab | - | Checking code | 23:14 |
TITLE: 08/06 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Observing at 151Mpc
OUTGOING OPERATOR: Ryan S
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 19mph Gusts, 14mph 3min avg
Primary useism: 0.07 μm/s
Secondary useism: 0.11 μm/s
QUICK SUMMARY:
IFO is in NLN and OBSERVING as of 22:22 UTC (24hr 45 minute lock)!
IFO continues to be very well behaved. Nothing of note.
Yesterday, we installed the BTRP (Beam Tube Roughing Pump) adapter flange on the 13.25" gate valve just to the -X side of GV13. This included installing a 8" GV onto the roughing pump port of the adapter, moving the existing gauge tree onto the new adapter, and installing a 2.75" blank on an unused port. All of the new CF joints were helium leak tested and no signal was seen above the ~9e-11 torrL/s background of the leak detector.
The assembly is currently valved out of the BT vacuum volume via the 13.25" GV, and is being pumped down via small turbo and aux cart. Therefore, the PT-343 gauge reading is only reporting on the BTRP assembly pressure, not the main BT pressure, so it can be ignored until further notice of it being vavled back in. This system has been pumping via aux cart or leak detector since ~2pm yesterday, and will continue to be pumped until it is in the pressure range of the BT volume. The aux cart is isolated by foam under the wheels, but some noise may be noticed by DetChar folks, hence the DetChar tag on this report.
A before - after pair of photos. As the conductance is very bad in this complex volume, we're aiming to pump it until next Tuesday. The estimated pressure rise of the main volume after valving in this small volume next Tuesday is less than E-12 Torr (after equalizing) - in other words, negligible.
Some backstage snapshots of the great teamwork of Travis, Janos, and me on installing these: Pic. 1 - "before"; 2,3 - 90% complete.
As of Tuesday, August 12, the pumps have been shut off and removed from this system, and the gauge tree valved back in to the main volume. Noise/vibration and pressure monitoring at MX should be back to nominal.
LOTO was applied now both to the handlers of the hand angle valve and the hand Gate Valve. Also, components have been added to the header, only 1 piece away from the booster pump.
DQ Shifters: Riley McNeil and Emil Lofquist-Fabris.
Daily observing duty cycle: 57.91%, 38.96%, 38.57%, 51.84%, 53.67%, 89.90%, 55.83%. Week average: 55.24% Observing.
This week was plagued by earthquakes, most notably the 8.8 magnitude earthquake from Russia and its subsequent aftershocks.
These really hindered the duty cycle of the detector.
The elevated ground motion in the earthquake band appears to be related to light scattering just above 20 Hz.
BNS range was consistently around 150-155 Mpc throughout the week, with 1 exception being on Sunday, when the detector ran without the squeezer for 2 and a half hours, dropping the range by about 15 Mpc.
There were also multiple days where the SQZ had issues staying locked, causing the detector to drop out of observing.
Throughout the shift there has been recurring glitching/noise in the 20-40 Hz range, seen both in the glitch and strain plots. However, they were less significant in the last two days.
This has been seen in previous shifts, however relatively inconsistently.
There was a recurring spike in noise in the H1 Y-manifold beam tube motion [X] at the exact same time every day this week (right after 17:00)
For the first 4 days of the shift, there was a recurring noise from ~11:00-13:00 in the corner station accelerometers (all degrees of freedom), however starting Friday it stopped showing up.
There was a low chi-squared PyCBC trigger that appears to be a blip, with the new SNR being the same as its original SNR on August 2.
See the full report here: https://wiki.ligo.org/DetChar/DataQuality/DQShiftLHO20250728
The spike in the YMAN accelerometer is caused by the daily dewar fill noise at the Y-manifold cryopump. The noise at 20 Hz (and the harmonic at 40 Hz) shown in your Friday Lock/Strain plot is likely from an AC unit housed inside the VPW (see alog 86257).
19:50 UTC
While I was trying to damp the highest modes, the pair around 1008 on ETMX (newish modes that were discovered in 2023 alog68650) which have been above 10^-16 on DARM I noticed that the other pair from ETMY (16 & 17) were not being monitored. I went into SUSPROC and unmonitored FM1, and the gain for the BL and RMSLP banks for EY 16 & 17, I turned on FM1 then ramped up the gains starting with BL then RMSLP, then I accepted and remonitored them all.
State of H1: Observing at 150Mpc
Quiet morning with H1 staying locked throughout; current lock stretch is almost up to 21 hours. There was one brief drop from observing at 15:34 UTC when the SQZ PMC unlocked, but everything recovered automatically and H1 resumed observing a few minutes later.
Oli, Ivey, Edgard.
We used Oli's measurements from [LHO: 86204] to do an OSEM calibration for the PR3 M1 OSEMs. Here are the outputs of the calibration script.
_______________________________________
OSEM calibration of H1:SUS-PR3
Stage: M1
2025-08-05_1700 (UTC).
The suggested (calibrated) M1 OSEMINF gains are
(new T1) = 1.770 * (old T1) = 2.055
(new T2) = 1.547 * (old T2) = 1.544
(new T3) = 1.443 * (old T3) = 1.511
(new LF) = 1.590 * (old LF) = 1.862
(new RT) = 1.774 * (old RT) = 2.063
(new SD) = 1.543 * (old SD) = 1.639
To compensate for the OSEM gain changes, we estimate that the H1:SUS-PR3_M1_DAMP loops must be changed by factors of:
L gain = 0.596 * (old L gain)
T gain = 0.648 * (old T gain)
V gain = 0.617 * (old V gain)
R gain = 0.617 * (old R gain)
P gain = 0.670 * (old P gain)
Y gain = 0.596 * (old Y gain)
The calibration will change the apparent alignment of the suspension as seen by the at the M1 OSEMs
NOTE: The actual alignment of the suspension will NOT change as a result of the calibration process
The changes are computed as (osem2eul) * gain * inv(osem2eul).
Using the alignments from 2025-08-05_1700 (UTC) as a reference, the new apparent alingments are:
DOF Previous value New value Apparent change
---------------------------------------------------------------------------------
L -57.1 um -33.6 um +23.5 um
T -101.3 um -65.6 um +35.7 um
V 62.4 um 36.6 um -25.8 um
R 433.5 urad 225.7 urad -207.8 urad
P -631.8 urad -406.5 urad +225.2 urad
Y -166.7 urad -76.1 urad +90.5 urad
We have estimated a OSEM calibration of H1 PR3 M1 using HAM2 ST1 drives from 2025-05-21_0000 (UTC).
We fit the response M1_DAMP/HAM2_SUSPOINT between 5 and 15 Hz to get a calibration in [OSEM m]/[GS13 m]
This message was generated automatically by OSEM_calibration_SR3.py on 2025-08-06 01:07:57.985744+00:00 UTC
%%%%%%%%%%%%%%%%%%%%%%%%%%%%
EXTRA INFORMATION
The H1:SUS-PR3_M1_OSEMINF gains at the time of measurement were:
(old) T1: 1.161
(old) T2: 0.998
(old) T3: 1.047
(old) LF: 1.171
(old) RT: 1.163
(old) SD: 1.062
The matrix to convert from the old Euler dofs to the (calibrated) new Euler dofs is:
+0.596 -0.0 +0.0 -0.0 +0.0 -0.003
+0.0 +0.648 -0.0 +0.0 +0.0 -0.0
-0.0 +0.0 +0.617 -0.004 +0.001 +0.0
+0.0 +0.0 -0.748 +0.617 -0.007 -0.0
+0.0 +0.0 +0.517 -0.036 +0.67 -0.0
-0.407 +0.0 -0.0 +0.0 -0.0 +0.596
The matrix is used as (M) * (old EUL dof) = (new EUL dof)
The dof ordering is ('L', 'T', 'V', 'R', 'P', 'Y')
The calibration values posted here are correct, but the theoretical alignment values are incorrect. See the corrected post from Sep 26th, 2025.
[CORRECTED LOGPOST LHO: 87160]
I posted LHO:81917 regarding the calibrated ASC coupling functions. At the time, my results seemed wildly large and I was certain I had made some calibration error somewhere, and indeed I had. Lee reached out last week since he is working on something similar for his optimal controls work, see LLO:77901. These are the calibration errors I made:
The full counts of drive to Nm of torque conversion factor is therefore: (20 / 2**20) * 0.268e-3 * 0.0309 * 70.7e-3 * 4 * 3.5355 * 4 = 6.317e-10 Nm/ct
Lee also pointed out instead of using the modeled free suspension plant, I should be using the radiation pressure modified plant. This is correct, however for the purposes of calibrating the coupling function the effect is mostly the same, since we know that the rad/Nm transfer function is the same at 10 Hz within a few percent for zero power and high power.
However, for completeness, and because it matters for other calibrations, I did this instead:
The end result is much more sensible, resulting in a coupling function around 30 Hz that is about 1 mm/rad for both pitch and yaw. This is still "high" in the sense that Matt and Lisa assumed a coupling on the order of 0.1 mm/rad in T0900511.
I went a step further to check the linearity of the coupling. I measured the transfer function of ASC to DARM during the noise budget injection times. However, the noise budget is usually calculated with an excess power projection, so we have both quiet and injection times taken. Using the same calibration method, I compare the excess power coupling function with the linear transfer function coupling function. They appear to be nearly the same, showing that the ASC coupling is dominated by linear behavior.
Back in March 2024, Gabriele, Louis, and I did several tests of the DHARD Y coupling while adjusting the ITMY Y2L gain (centering of the beam on ITMY in yaw) and the AS A yaw WFS offset (centering of the beam on the DHARD Y sensor). I used the method above to calibrate the measured couplings so we can better understand the effect of each.
First, I used data where Gabriele and I adjusted the ITMY Y2L gain and measured the DHARD Y coupling. I calculated the linear coupling function at each Y2L gain, so we could observe the effect of the phase of the coupling as the Y2L gain is changed. Using the a2l_lookup matlab function in /opt/rtcds/userapps/release/isc/common/scripts/decoup/BeamPosition, I calibrated the A2L gains into spot position in mm from the center.
While adjusting the beam position reduced the DHARD Y coupling above 25 Hz reduced as the beam moved from about 6.4 mm to 4.4 mm from center, the low frequency steep coupling appears to increase.
The flat coupling was overall higher at this time (at best reaching about 5 mm/rad), possibly because the other test mass A2L gains were not completely optimized.
Next, Gabriele and Louis varied the AS A WFS yaw offset between -0.2 and -0.1 and measured the same coupling. I again calculated the linear coupling function for each step. It appears that both the magnitude and the frequency dependence of the steep coupling varies with the offset. At an offset of -0.2, the coupling is more like 1/f^2, but at an offset of -0.1 it is more like 1/f^4.
We are currently operating with zero WFS yaw offset.
Today, Sheila and I decided to increase the ETMX ESD bias voltage. We would like to operate at a higher bias for a short period to see if the extra actuation range allows us to survive the ETMX glitch locklosses. However, we also wanted to understand what effect this has on our range.
Sheila made small steps to increase the ETMX bias voltage and adjusted the L3 drivealign gain accordingly. After every step, I measured the DARM open loop gain and we adjusted the drivealign gain further to maintain the DARM UGF. Once we doubled the voltage, we further adjusted the drivealign gain to bring kappa TST to one. It's important to note that we saw that the correction factor required to maintain the UGF (at 70 Hz) was slightly different than the correction factor required to bring kappa TST back to 1 (measured at 17.6 Hz).
We took a PCAL broadband measurement at the regular and double bias configurations (documented here). Even with kappa TST near 1, there was a small frequency-dependent difference between the two measurements.
Sheila then took us back and forth from the double bias to regular bias states so we could get some noise comparison times to determine if the noise is worse with double bias.
| Times in UTC | Start | End |
| double bias | 17:41:58 | 18:03:37 |
| single bias | 18:08:20 | 18:17:30 |
| double bias | 18:18:37 | 18:26:37 |
| single bias | 18:27:40 | 18:35:40 |
I exported the PCAL broadband injections and used them to calibration GDS strain for the four times above into PCAL meters. The noise from 15-400 Hz looks to be the same for each time, so I don't think there will be a significant impact to the sensitivity if we double the bias.
I ran a linear regression fit on the voltage and drivealign data from our steps, using this document as reference. I was able to fit alpha - gamma (slope) and the beta values (y-intercept). I calculate alpha - gamma = 9.14e-10 N/V^2 and beta - beta2 = -4.08e-8 N/V
We are planning to go to this double bias for some time to see if reduces the number of ETMX glitch locklosses.
We've done this change with a guardian shell. I've attached a text file with options that people can use to do these steps, or revert them.