I updated the POP_A P and Y offsets so the DRMI ASC will take us closer to where the full IFO ASC will take us
DOF | Old | New |
P | 0.09 | 0.1 |
Y | 0.35 | 0.15 |
This was reverted - the DRMI alignment and full IFO alignment are not the same. Maybe related to the ITMX P2L gain change we put in which adjusts the pitch of the PRM in 2W full lock?
FAMIS 25805
pH of PSL chiller water was measured to be between 10.0 and 10.5 according to the color of the test strip.
Betsy, Ryan S, TJ
We did our first walk through after the vent, but next week there will definitely be more to sweep that we either missed or that we said we will hold off a week on. We focused on the most egregious items.
Jonathan, Nyath
As per WP 12580 we have replaced the GC switch which interfaces with CDS. This is in response to the need to cycle the switch twice on Friday.
Unfortunately this took more work than expected. The first switch we tried was not passing data between the CDS router and the GC core. So we are running a smaller spare CDS switch with POE + 10Gb capability to service the control room phones, the control room computers, and the DMT interface.
We have two fiber pairs going to the GC core switch. We typically run them as an aggrigated link. However for testing we have split that up and are running one pair to the active switch and have the other fiber pair to test another switch.
This work resulted in minor outages to the DMT and control room. The largest outages being to the non-operator phones.
We will keep the work permit open for a bit.
Attatched to this alog are omicron glitch rate comparions, as a function of frequency and SNR, between O4a and O4b. Here, I used roughly ~ 3425 hours of observing time for O4a and O4b (H1:DMT-ANALYSIS_READY:1 flag). The specific observing times used were:
O4a: 2023-06-24 20:00:00 - 2024-01-17 00:00:00 (~3422 hours observing)
O4b: 2024-04-10 00:00:00 - 2025-01-28 17:00:00 (~3428 hours observing)
The SNR and frequency of the omicron triggers gathered were 7.5 < SNR < 500, and 10 Hz < frequency < 1024 Hz. I find that the glitch rate in O4b is significatly less than O4a. In O4a, there was a lot of non-stationary noise from ~10-50 Hz (see alogs 71005 & 71092), which is why the rate was so high. For frequencies below 50 Hz, the glitch rate per hour went from roughly ~16.7 in O4a to ~2.5 in O4b. For SNR below 50, the glitch rate per hour went from ~36 per hour in O4a to ~9 per hour in O4b.
Tue Jun 03 10:11:02 2025 INFO: Fill completed in 10min 59secs
Hello! I have been working on eventually calculating how much force is being applied to three stages of the quadruple pendulum. The channels I am currently plotting in the figures attached are the DARM control signal (H1:CAL-CFTD_DELTAL_CTRL_DBL_DQ), the penultimate mass control signal (H1:CAL-CFTD_DELTAL_CTRL_PUM_DBL_DQ), the upper intermediate mass control signal (H1:CAL-CFTD_DELTAL_CTRL_UIM_DBL_DQ), the top test mass control signal (H1:CAL-CFTD_DELTAL_CTRL_TST_DBL_DQ), the external excitation signal (H1:CAL-CFTD_DELTAL_EXTERNAL_DQ) and Pcal y (H1:CAL-PCALY_RX_PD_OUT_DQ) - I should include Pcal X next time. By plotting these channels I can map out how much each stage of the quadruple pendulum is moving (or being actuated upon), the Pcal injections, and eventually compare the force needed to control each stage to keep our interferometer locked. Right now I am plotting the meters per root Hz for each channel. I am also applying an anti-whitening filter so that I can convert the signals from counts back into the physical displacements. The path to the file to plot these figures is: /ligo/home/caroline.capuano/Force_on_ETMX_for_each_stage/phase_and_mag_of_h.py All you need to do is run "python phase_and_mag_of_h.py" and it should produce both plots. Currently I am taking data from LIGO Hanford at the GPS start time of 1425831025 for a duration of 1000 seconds. There is a weird bump around 100 Hz for the external excitation signal, so Craig suggested I find another time of when we were locked and compare to see if the hump is still present. To do next: - figure out what filters to divide by so that I can calculate the force being applied to the three stages aka N/rtHz. - maybe try quick_psd instead of welch's method and see if that makes a significant difference
Two index number changes this morning:
TITLE: 06/03 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Planned Engineering
OUTGOING OPERATOR: TJ
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 5mph Gusts, 2mph 3min avg
Primary useism: 0.02 μm/s
Secondary useism: 0.27 μm/s
QUICK SUMMARY:
IFO is in DOWN for PLANNED ENGINEERING
Today is a light maintenance day in with the plan being to continue locking H1 to NLN.
The highest state we are able to get to is: LOWNOISE_LENGTH_CONTROL.
Workstations were updated and rebooted. This was an os packages update. Conda packages were not updated.
After opslogin0 was rebooted I started the two temporary EPICS IOCs to green up the EDC and restore the HAM1 gauge signal
digivideo_dummy_ioc: 1 windows (created Tue Jun 3 06:53:08 2025)
vac_ham1_pressure_converter_ioc: 1 windows (created Tue Jun 3 06:54:12 2025)
TITLE: 06/03 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Planned Engineering
INCOMING OPERATOR: None
SHIFT SUMMARY:
Just had another lockloss so I'm just putting the detector in IDLE for the night. I have a list of things from Elenna to check/try with relocking, but I won't be able to get to any of them before the end of my shift, so they can be checked tomorrow morning. This last lockloss was during OFFLOAD_DRMI_ASC while I was trying to adjust SRM, although I don't think I caused the lockloss? It took a while for DRMI to catch this time, so maybe running an initial alignment is warranted. The highest state we were able to get to today was LOWNOISE_LENGTH_CONTROL.
The list Elenna gave me is:
LOG:
23:00UTC Commissioning and sitting in POWER_10W
23:20 Started trying to increase power
01:49 Lockloss from LOWNOISE_LENGTH_CONTROL while sitting there running measurements
- Started a manual initial alignment
- Stopped at PRX_LOCKED, touched up PRM, then finished IA
- Stopped at OFFLOAD_DRMI_ASC, touched up SRM, then continued
- Lockloss in DRMI_TO_POP
- Probably due to DRMI alignment not being the greatest
- Stopped at OFFLOAD_DRMI_ASC, touched up SRM, SR2, and PRM, then continued
- Lockloss in LOWNOISE_ESD_ETMX due to a CHARD P ringup that started in TRANSITION_FROM_ETMX
- Lockloss from OFFLOAD_DRMI_ASC while I was trying to touch up alignment using SRM. Not sure if my fault?
Writing this alog on behalf of most of the control room...
After we redid the input matrix for CHARD and INP1 10W, we checked the PRC2 and INP1 bandwidth. We were also concerned about the overall gain of CHARD P and Y since they seemed to be way too low
We decided to power up anyway, and saw that the pitch ADS was able to run fine, now that the CHARD pitch gain was nominal. However, yaw ADS still had problems during move spots.
Everything looked good, so I took us up in power from 25W to 60W, stopping frequently to check for instabilities. We made it, but again the ADS was unstable, so Georgia used the Camera servo guardian to move off the ADS to camera servos, and everything was fine.
I stepped through lownoise ASC by hand, skipping the lownoise steps of CHARD P and Y since those gains were not nominal.
Lots of the of the usual wobbly stuff in the ASC and buildups at high power, but the overall alignment and control looks good: PRG is still around 50 at full power.
We then ran through lownoise coil drivers and the ETMX ESD transition. We had one guardian error at the end of TRANSITION FROM ETMX due to divide by zero error since the convergence checker looks for something that is like [ADS error signal / ADS CLKGAIN] and the ADS CLKGAINs were zero. Georgia and I fooled the guardian by setting the CLKGAINs to 1 momentarily, and then undoing them once the state completed.
We ran all the way through LOWNOISE LENGTH CONTROL, although the LSC feedforward is no longer well-tuned, so I turned it off momentarily so we could check OLGs.
The LSC feedforward is currently so bad that we should go from-scratch when we retune it instead of the iterative method.
We had a fast unknown lockloss while sitting in this state- no one was doing anything and we don't see an obvious cause.
We think we have properly SDFed and guardianized all changes from today.
My only worry: we were not able to raise the CHARD Y gain until we reached maximum power, but obviously we are having ADS stability issues since this gain is too low. Currently I have set the guardian to have what I think is the "correct" CHARD Y gain (300 once all loops are closed), but if it's too high, drop it back to 3.
Recommended to do list:
Oli and I are trying out relocking, and both sitting at 2W and sitting at 25 W (before move spots), I cannot raise the CHARD Y gain beyond 3 without causing some slow growing ~0.8 Hz oscillation in CHARD Y. We will try full power up again with low CHARD Y gain. Turns out the CHARD Y gain was not actually set to 300 at 2W (I only updated lscparams, not ISC_LOCK).
After MOVE SPOTS and reducing modulation depths (but before the rest of the power up), I tried again to raise the CHARD Y gain- same problems.
But once MAX POWER gets us to 60W, I can raise the gain no problem!
I edited MAX POWER to change the CHARD Y gain right at the end of the state (I think).
In terms of setting the time on the ASC convergence in MOVE SPOTS, YAW3 (ITMX spot feedback to PRM) is the culprit that is taking forever.
Oli just took a look back- we usually spend about 5 minutes in move spots, and tonight it is taking more than 10 minutes.
We were able to run through LOWNOISE ASC guardian state fine, so the edits described above work!
We lost lock from a 1 Hz DHARD P ring up that began during the "TRANSITION FROM ETMX" state.
When we went through this state previously and successfully, we were running camera servos instead of ADS. I wonder if that's related to this lockloss.
Changed the DARM_OFFSET ISC_LOCK state number to be in order, after ENGAGE_ASC_FOR_FULL_IFO
This change was reverted - alog84741
Jennie W, Sheila, Elenna
In order to get data for mode-matching and for Elenna to get data to calibrate sideband heights we ran some mode scans after the SR3 heater was turned on last night.
16:55:24 UTC Carried out single bounce OMC scan at 10W PSL input with sensor correction on HAM6 on, high voltage on for PZT driver in HAM6, sidebands off , SRM mis-aligned, ITMY mis-aligned, DC 3 and 4 on, OMC ASC on.
Excitation freq changed to 0.005 Hz as the top peak of the TM00 mode looked squint so could have been saturating. Lowering this frequency prevented this.
Ref 15-17 corresponds to dcpd data, pzt exc signal, pzt2 dc monitor.
Then mis-aligned ITMX and aligned ITMY (Sheila had to re-align SR2 to centre on ASC-AS_C).
Measurement starts at 17:08:18 UTC.
Ref 18-20 corresponds to dcpd data, pzt exc signal, pzt2 dc monitor.
Traces saved in 20250516_OMC_scan.xml. The top left plot is the first scan bouncing beam off ITMX, the second scan is the bottom right bouncing off ITMY.
The top right is the two plots of the PZT2 DC voltage monitor. That is, the current voltage applied to the PZT. The bottom left is the plot of the voltage ramp applied to the PZT2 on the OMC for this measurement.
The ndscope attached shows the power in mA transmitted through the OMC on the top, then the PZT used for the scan DC voltage underneath, then the input PZT voltage underneath that, then the reflected power from the OMC in mW, then at the bottom the SR3 heater element temperature in degrees.
Elenna did two more scans in single bounce with sidebands back on and different modulations depths in each.
See Elenna's comment on her previous measurement where this saturation happened.
Turn off the sidebands - instructions in this alog.
Sheila and I ran one more OMC scan with sidebands off after OM2 heated up. Attached is the screenshot with scans off both ITMX and ITMY, data is saved in [userapp]/omc/h1/templates/OMC_scan_single_bounce_sidebands_off.xml
I also ran two OMC scans, single bounce off ITMY, 10 W input, with the sidebands ON. One measurement I ran with the sidebands set to 23 dBm and 27 dBm (9 and 45 MHz) and another set to 20 dBm and 21 dBm (9 and 45 MHz). I will use these measurements to calibrate the modulation depth. Data saved in /opt/rtcds/userapps/release/omc/h1/templates/OMC_scan_single_bounce_RF_cal.xml
SR3 heater was on for this measurement but it should have little effect on my results.
Looked closer at these HWS signals during SR3 heater heat up and cool down. In all these plots, the two t-cursors are used as the reference and shown HWS live image.
Some strange things:
TJ, Camilla, Sheila
TJ and Camilla got the HWSs working, and now we turned on the SR3 heater at 15:54 UTC, 2W requested power. This is to do a check of the SR3 heater calibration and range similar to 27262
SR3 heating up can be seen on the HWS signals but is not particulatly clear, see attached.
Looking at when this test was done at LLO, the lens changing happened over a period of three hours and the lens power increased in the same direction on both HWS, so its possible our HWS are not a good witness for the SR3 curvature change.
Aidan calculated 2.45 uD/W at LLO, and we get 9.44 uD/W (from the H1:TCS-ITM{Y,X}_HWS_PROBE_SPHERICAL_POWER trends with an estimated noise of 4.48e-12uD/W.
Looked closer at these HWS signals during SR3 heater heat up and cool down. In all these plots, the two t-cursors are used as the reference and shown HWS live image.
Some strange things:
With the numbers from ITMY HWS only, and looking at the 3hr 11 m cooldown in Camilla's photo, the lens change is 6.68e-6 Dioptres/W taking into account that the HWS beam passes twice through SR3.
After talking with Camilla, she reminded me the change in RoC (delta R) =/= 2/(delta D),
where D is defocus (1/focal length).
but instead delta R = 2/(2/R + delta D) - R
Where R=36.013m is given in https://git.ligo.org/IFOsim/ligo-commissioning-modeling/-/blob/main/LHO/yaml/lho_O4.yaml?ref_type=heads
delta R comes out as 4.3mm +/- 0.18 mm (which is the same order of magnitude as the change Aidan measured in alog #27262 at LLO).
The error was estimated from looking at the noise on the spherical power and propagating through the calculation of delta R.