Displaying reports 141-160 of 86532.Go to page Start 4 5 6 7 8 9 10 11 12 End
Reports until 08:25, Wednesday 28 January 2026
H1 SEI
oli.patane@LIGO.ORG - posted 08:25, Wednesday 28 January 2026 (88932)
BRS Drift Trends - Monthly FAMIS

Closes FAMIS#38813, last checked 88386

BRS Driftmon
Auxiliary BRS Channels

Everything is looking normal

Images attached to this report
H1 General
oli.patane@LIGO.ORG - posted 07:32, Wednesday 28 January 2026 (88931)
Ops Day Shift Start

TITLE: 01/27 Day Shift: 1530-0030 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Planned Engineering
OUTGOING OPERATOR: None
CURRENT ENVIRONMENT:
    SEI_ENV state: MAINTENANCE
    Wind: 4mph Gusts, 3mph 3min avg
    Primary useism: 0.03 μm/s
    Secondary useism: 0.33 μm/s 
QUICK SUMMARY:

LVEA is still LASER HAZARD

H1 ISC (ISC)
keita.kawabe@LIGO.ORG - posted 21:00, Tuesday 27 January 2026 - last comment - 06:56, Wednesday 28 January 2026(88927)
JAC EOM update Tue/Jan/27 (Elenna, Keita, phone consultation with Valera)

Summary:

A day of success.

Comments related to this report
keita.kawabe@LIGO.ORG - 21:36, Tuesday 27 January 2026 (88928)

How crystal mounting was done.

We did "in-between" method (alog 88900) and inserted two pieces of 3/8IDx5/8ODx0.025" thick shim washers between the front plate and the input side plate.  shim_washers_spacers.jpg shows the washers and the front plate before the rest of the EOM structure is placed on top. Note that the front plate still has the alumina piece on top, not the RTP. Important points in this picture:

  1. We're using two pieces of alumina pieces as a convenient 4mm thick shim to raise the front plate. It doesn't have to be alumina pieces, but the front plate must be raised enough so the shim washers "clear the ground".
  2. Three set screws are pre-adjusted so each sticks out just shy of 3.5mm. This is the height of the crystal (4mm) minus the depth of the shallow groove (nominally 0.02" or 0.508mm). This made it somewhat easier to to make sure that there's a good contact between the crystal and the metals.

(Added later: If I were to do this again, I'll set the set screws with alumina piece in place such that all touch the board when there's a good contact between board/plate/alumina (of course no indium). Insertion of indium foil with the real RTP later will automatically ensure that the screws are just shy.)

Next we cut a 40mmx4mm piece of indium sheet with a clean pair of scissors and installed it in a groove in the front plate. I tried to set the edge of the sheet to be 7.6mm from the outside edge of the front panel (this is 7mm plus the thickness of 0.025" washer). Judging from indium.jpg, I was mildly successful, maybe it's more like 7.4mm but it's not 7mm nor 8mm.

rtp.jpg shows the side view of the crystal. Maybe it's hard to see but it's wedged, in this picture the shortest face is down, the longest side is up.

I placed the crystal on top of the indium sheet, making sure that the edge of the crystal is well aligned with the edge of the indium as good as I can. We also made sure that the shortest face mates with the front panel. You cannot see any of that in the crystal_installed.jpg but you can at least see that the crystal is there.

Then we went through the same procedure we've already done more than several times, i.e. tighten the screws on the input panel until the panel touches the washer and the washer touches the front panel, tighten the scrwes on the output panel so the screws touch that panel, then go balanced tightening, moving just a tiny amount at a time, always applying small downward pressure for the EOM side/board/bottom assy otherwise the assy will shift when the screws are tightened. When all of the screws are tightened stronger than finger tight, screws on the input side are tightened just a bit more. After this, neither Elena nor I weren't able to undo screws by finger.

Sorry no picture of the assembled unit.
 

Images attached to this comment
keita.kawabe@LIGO.ORG - 23:35, Tuesday 27 January 2026 (88929)

Tuning is done, larger capacitance than obtained before with alumina, looks good. (But why do the dips have to be so narrow?)

We noticed that the frequencies were lower than what we have previously obtained with alumina, i.e. the capacitance is bigger. This is probably a good sign even though we don't know if this is due to the indium or something else. Especially, 118MHz dip was a MHz or two lower than nominal.

We were able to tune all four frequencies using trim cap, except that the trim cap for 45.5MHz hit the minimum and we could not increase the frequency any more, so we bent the winding of the coil a bit to spread loops apart. Below is the table of center frequencies (actual vs nominal). In the attached photos, cursor is placed close to the nominal frequency. They all look good in that the frequency is close enough to nominal that we're only loosing less than a dB, but the resonances are all very narrow (for my preference, anyway). The Q values are from 640 for 9MHz to 1300 for 118MHz, going higher as the frequency. A small change in frequency will result in a big degradation in the modulation depth.

(Added later: Read Valera's entry below, thanks Valera! The numbers here are not the real Q, they should be smaller. To make it more embarrassing, I somehow mixed up 3dB and 6dB. Given that all dips are smaller than -20dB, a quick thing to do is probably to define the width of the peak as full width of the -3dB points in S11, not +3dB points from the bottom but really -3dB measured from 0dB full reflection. If you do that the numbers are more like 100 instead of 1000.)

If you look at the pictures, you'll also notice that the reflection dips at the center are -23dB (9MHz), -24.5dB (24MHz), -23dB (45MHz) and is -25dB (118MHz) so a bit smaller than 10% in amplitude is coming back. It's not really matched to 50 Ohm transmission line, and that on its own is OK, but because of that, I wonder if we can add a bit of resistance to bring down Q values without any negative impact (like worse matching with increased reflections) in the future design. 

Tuned center Nominal Full width of 6dB points from the bottom / Q
9.0995 9.100230 14.3k / 636
24.07705 24.078360 29.7k / 810
45.5043 45.50115 57k / 798
118.3055 118.30299 89k / 1329

After this first round of tuning, three set screws on the front plate were all extracted, and there was no change in the tuning of 118MHz dip.

I changed the orientation of the EOM and the frequency jumped a bit

Up to this point, tuning was done with the front plate facing down and put on the ceramic insulator placed on the EOM base (because it's convenient to access trim caps that way).

When I changed the orientation of the EOM so the front plate becomes upfront (i.e. like intended), the frequency of 118MHz dip shifted a bit, from 118.3055MHz to 118.31745MHz, it's just 12kHz shift so not the end of the world but it's still meaningful. Maybe it's the interaction of the magnetic field from the coil and the metals nearby?

Then I tapped the front plate and side plates and it shifted again, fortunately by smaller amount (from 118.31745 to 118.3113MHz, a negative 6kHz jump).

What we'll do tomorrow is to fully assemble the unit, tune it again as good as we can, then tap and retune if necessary. Hopefully, tapping enough and things will settle to the bottom of the potential.

Once the EOM goes into chamber we'll measure the resonances again, and we might have to retune in chamber.

Images attached to this comment
valery.frolov@LIGO.ORG - 06:56, Wednesday 28 January 2026 (88930)

I was also wondering why the S11 (return loss) is narrower then the transmission curve back when we did the prototype testing at LLO. So I did the math myself - the attached plot shows the calculated curves for voltage across the crystal for 1 W incident RF power and S11 for 9.1 MHz (similar for other f's). Initially I also made the same mistake estimating the Q - the Q is actually about 100 not ~1000 as one can see from the transmission curve (voltage on the crystal).   

Images attached to this comment
H1 AOS
masayuki.nakano@LIGO.ORG - posted 18:55, Tuesday 27 January 2026 (88926)
HAM1 alignment work

[Jennie, Jason, Masayuki]

Summary:

We aligned the HAM1 output beam to the IMC and verified the power transmission through HAM2. The beam path through JAC_L2/L3 was centered, and alignment to the IMC was improved. Preparation for EOM installation is nearly complete, with final measurements planned for tomorrow.


Details:

 

H1 CAL
anthony.sanchez@LIGO.ORG - posted 17:42, Tuesday 27 January 2026 (88924)
PCAL EX End Station Measurement.

Dripta & I went to the EX to do a PCAL End station measurement followed by a TX module maintenance.

Obligitory Beam spot pic.
We followed T1500062-V21, with out much deviation until the measurements were finished. We did continue on with a TX module maintenance that we have not yet finished yet. Our plan is to go back tomorrow to finish the OLTF Optical Follower Servo measurement. We did leave the LASER HAZARD STATUS at EX in SAFE

The ES measurement went smoothly.
Beam spot after ES measurement & TXmodule maintence!

python generate_measurement_data.py --WS PS4 --date 2025-11-03
Reading in config file from python file in scripts
../../../Common/O4PSparams.yaml
PS4 rho, kappa, u_rel on 2025-11-03 corrected to ES temperature 299.5 K :
-4.7017855975867215 -0.0002694340454223 2.686163396659873e-05
Copying the scripts into tD directory...
Connected to h1daqnds1
martel run
reading data at start_time:  1453573090
reading data at start_time:  1453573550
reading data at start_time:  1453573950
reading data at start_time:  1453574260
reading data at start_time:  1453574700
reading data at start_time:  1453575050
reading data at start_time:  1453575167
reading data at start_time:  1453575840
reading data at start_time:  1453576170
Ratios: -0.4588903912882054 -0.46880057152484483
writing nds2 data to files
finishing writing
Background Values:
bg1 =        9.720121; Background of TX when WS is at TX
bg2 =        4.686352; Background of WS when WS is at TX
bg3 =        9.770692; Background of TX when WS is at RX
bg4 =        4.628189; Background of WS when WS is at RX
bg5 =        9.797052; Background of TX
bg6 =        0.801247; Background of RX

The uncertainty reported below are Relative Standard Deviation in percent 

Intermediate Ratios
RatioWS_TX_it      = -0.458890;
RatioWS_TX_ot      = -0.468801;
RatioWS_TX_ir      = -0.453881;
RatioWS_TX_or      = -0.463503;
RatioWS_TX_it_unc  = 0.073150;
RatioWS_TX_ot_unc  = 0.076593;
RatioWS_TX_ir_unc  = 0.078168;
RatioWS_TX_or_unc  = 0.089042;
Optical Efficiency
OE_Inner_beam                      = 0.989262;
OE_Outer_beam                      = 0.989063;
Weighted_Optical_Efficiency        = 0.989162;

OE_Inner_beam_unc                  = 0.049361;
OE_Outer_beam_unc                  = 0.054133;
Weighted_Optical_Efficiency_unc    = 0.073259;

Martel Voltage fit:
Gradient      = 1636.767509;
Intercept     = 0.537748;


 Power Imbalance = 0.978861;

Endstation Power sensors to WS ratios::
Ratio_WS_TX                        = -1.077945;
Ratio_WS_RX                        = -1.393587;

Ratio_WS_TX_unc                    = 0.045600;
Ratio_WS_RX_unc                    = 0.039824;

=============================================================
============= Values for Force Coefficients =================
=============================================================

Key Pcal Values :
GS           =      -5.135100; Gold Standard Value in (V/W)             
WS           =      -4.701786; Working Standard Value             

costheta     =      0.988362; Angle of incidence
c            =      299792458.000000; Speed of Light
             
End Station Values : 
TXWS         =        -1.077945; Tx to WS Rel responsivity (V/V)
sigma_TXWS   =        0.000492; Uncertainity of Tx to WS Rel responsivity (V/V)
RXWS         =        -1.393587; Rx to WS Rel responsivity (V/V)
sigma_RXWS   =        0.000555; Uncertainity of Rx to WS Rel responsivity (V/V)

e            =        0.989162; Optical Efficiency
sigma_e      =        0.000725; Uncertainity in Optical Efficiency

Martel Voltage fit : 
Martel_gradient         =        1636.767509; Martel to output channel (C/V)
Martel_intercept   =        0.537748; Intercept of fit of     Martel to output (C/V)

Power Loss Apportion : 
beta          =        0.998895; Ratio between input and output (Beta)  
E_T          =        0.994017; TX Optical efficiency 
sigma_E_T          =        0.000364; Uncertainity in TX Optical efficiency 
E_R          =        0.995117; RX Optical Efficiency 
sigma_E_R          =        0.000365; Uncertainity in RX Optical efficiency 

Force Coefficients : 
FC_TxPD          =        7.900822e-13; TxPD Force Coefficient 
FC_RxPD          =        6.178276e-13; RxPD Force Coefficient 
sigma_FC_TxPD          =        4.646331e-16; TxPD Force Coefficient 
sigma_FC_RxPD          =        3.364222e-16; RxPD Force Coefficient 
data written to ../../measurements/LHO_EndX/tD20260127/

 

Images attached to this report
Non-image files attached to this report
LHO General
ibrahim.abouelfettouh@LIGO.ORG - posted 16:44, Tuesday 27 January 2026 (88923)
OPS Day Shift Summary

TITLE: 01/28 Day Shift: 1530-0030 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Planned Engineering
INCOMING OPERATOR: None
SHIFT SUMMARY:

IFO is in IDLE for PLANNED MAINTENANCE

Good progress on activities today.

Other:

LOG:

Start Time System Name Location Lazer_Haz Task Time End
22:49 SAF LVEA IS LASER HAZARD LVEA YES LVEA IS LASER HAZARD \u0d26\u0d4d\u0d26\u0d3f(\u239a_\u239a) 16:49
15:44 FAC Nellie LVEA Y Technical Cleaning 17:06
15:51 SUS Betsy LVEA Y BSC2 Inspection 17:51
15:51 FAC Randy LVEA Y BSC2 Inspection 16:22
16:01 FAC Kim LVEA Y Technical Cleaning 17:06
16:33 FAC Richard LVEA Y BSC2 Inspection 17:07
16:33 FAC Randy LVEA Y BSC2 Inspection 23:04
16:42 PCAL Tony, Dripta PCAL Lab N PCAL Meas. 17:13
17:10 FAC Eric, Chris EX, EY, MX, MY N (YES EX) Air Handler and HVAC Maintenance 18:28
17:14 PCAL Tony, Dripta EX Y PCAL Measurement 19:17
17:16 EE Fil LVEA Y Moving electronics by HAM6 20:21
17:33 ISC Jennie LVEA Y Turning on light pipe 17:35
18:06 FAC Kim, Nellie LVEA Y Technical Cleaning 18:44
18:08 SUS Rahul LVEA Y HAM7 OPO 18:31
18:14 TCS Matt, Sophie JOAT/Vac-Prep Lab N CHETA 15:14
19:05 EE Marc HAM1 Y EOM Electronics 20:11
19:06 EE Daniel LVEA Y HAM6 Electronics 20:11
19:07 OPS Oli LVEA Y Reminding Daniel about a meeting 20:21
19:07 COC Masayuki, Jennie LVEA Y HAM1 EOM 20:45
19:08 SUS JAson LVEA Y HAM1 EOM 20:46
21:08 EE Fil LVEA Y HAM6 Electronics 23:06
21:11 PCAL Tony, Dripta EX Y PCAL Meas. 01:11
21:37 SUS Sheila, Rahul LVEA Y HAM7 22:48
21:45 COC Elenna, Keita Optics Lab N EOM 00:34
22:05 SUS-FAC Travis, Jim, Betsy, Gerardo, Tyler, Randy LVEA Y BSC2 Inspection 23:04
22:10 COC Masayuki, Jason LVEA Y HAM1 JAC 00:07
22:13 TCS Marc, Jennie Vac-Prep/JOAT Lab N CHETA Lable Table Cable 23:59
00:41 EE Marc LVEA Y EOM Reconnection 01:41

 

H1 SUS (SQZ)
jeffrey.kissel@LIGO.ORG - posted 16:09, Tuesday 27 January 2026 (88921)
Dramatic Improvement in H1SUSOPO TFs after Adjusting Cable Dressing; Still Some Work Tho
J. Kissel

Took a set of TFs after Rahul and Sheila re-dressed the cables surrounding the H1SUSOPO (LHO:88920). The TFs -- especially Y to Y look a *lot* better with the higher frequency modes re-aligning with historical measurements and the model. There's still some mode splitting in the lowest mode, that I suspect is the transverse/vertical/yaw system not quite yet as soft as it used to was. Rahul mentions they did *not* address the cables that were zip-tied to the H3/V3 spring post so that could be it.

We'll discuss and game plan more with the crew tomorrow.

Data templates saved here:
    /ligo/svncommon/SusSVN/sus/trunk/OPOS/H1/OPO/SAGM1/Data
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_L_0p02to50Hz.xml
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_P_0p02to50Hz.xml
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_R_0p02to50Hz.xml
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_T_0p02to50Hz.xml
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_V_0p02to50Hz.xml
        2026-01-27_2316UTC_H1SUSOPO_M1_WhiteNoise_Y_0p02to50Hz.xml
Again ran in the configuration where only the DOF being driven was undamped.
Non-image files attached to this report
H1 CDS (ISC)
filiberto.clara@LIGO.ORG - posted 16:05, Tuesday 27 January 2026 (88922)
Field Racks ISC-R5 and ISC-R6

WP 12991
WP 12994
D1200196 ISC-R5 Layout
D2400300 - ISC-R6 Layout
D1900511 - ISC/SQZ Wiring Diagram

In preparation for the installation of BHD, the following work was done to the HAM6 field racks:

1. ISC-R3 is now on its own set of power supplies for ±18V
2. ISC-R5 and ISC-R6 share a set of power supplies for ±18V
3. ISC-R3, ISC-R5, and ISC-R6 share a set of power supplies for ±24V
4. ISC-R5 was updated to D1200196-v15
5. ISC-R6 was updated to D2400300-v1

Racks are not complete. Missing electronics will be installed when available.

F. Clara, D. Sigg

H1 CDS
jonathan.hanks@LIGO.ORG - posted 15:45, Tuesday 27 January 2026 (88919)
WP 12998 cont Installing the new VM cluster

Test stand log book entries that document the setup and testing prior to production

Physical layout

The following components are racked together in rack 12.

  1. sw-msr-pve0 - switch that connects the nodes to each other and to the core.  It runs the internal cluster traffic, and contains the links to the outside world.
    1. Connected to the core via a lag.  I have spare ports in both the core and the switch so that I can increase the bandwidth if needed
  2. pve-node[0,1,2] - the nodes

Basic setup

When I updated the ipmi address in the bios I also did the install of the proxmox nodes.  I follow the basic routine in reworking the proxmox setup for pve-node0.

Repeat this for pve-node1 & 2, incrementing the ip addresses.

Cluster network configuration creation

Configured the niccluster0 interface on each node

Did the same on each node, and a ping test.

Cluster creation

On pve-node0 go to the datacenter / cluster and click on create cluster

Then on the other nodes to to datacenter / cluster and click join cluster

Support subscription activation and updates

Now that the basic pieces are in place and will not need a reinstall, it is time to enable the subscription on each node.

Go to each node to the subscription section and upload the subscription key.

Now run updates against the enterprise repo and reboot each machine.

Configure the ceph network

Repeat for all nodes

Install Ceph

Go to datacenter / ceph page.  When prompted, select install ceph

Clean up disks

We had used these machines for other testing in the test stand, we will go through and clean up the disks prior to use.

This was done on /dev/sdc and /dev/sdd on the systems

Create the Ceph OSD (Object Storage Deamon)

On each machine go to ceph/OSD

Repeat for /dev/sdd.

After a minute they should show up on the ui.

Add more Ceph monitors

Add pve-node1 and pve-node2 as ceph monitors and managers.

Add a Ceph pool

pve-node0 /ceph / pool

Setting up the VM data links, a bonded bridged network

Go to network / Create / Linux Bond

Create a data bridge, network / Create / Linux Bridge

Do this on each of the nodes.

Notes

When creating VMs we want to connect the network to vmbr1 and specify the vlan tag that should be used as this setup gives us access to more than one vlan.

H1 SUS (SUS)
rahul.kumar@LIGO.ORG - posted 10:59, Tuesday 27 January 2026 - last comment - 08:37, Wednesday 28 January 2026(88917)
HAM7 OPO health check investigation - took fresh pictures (in chamber) for comparison, looking for cable inteferances.

Jeff, Sheila, Rahul

Details about OPO health check issues (Yaw dof. - frequencies are off and unnecessary peak observed) is currently being analyzed - see Jeff's alog 88913.

This morning we discussed about possible cable interferences in OPO.

I went into the chamber and took fresh pictures of the OPO from several angles, focusing on cable routing, cable resting on the OPO etc - please find them attached below. I will compare them with the pictures posted in LHO alog 61643 (by Sheila in 2022) and look for possible culprits (a few of them already).

Moving cables could cause some misalignment, hence we will start doing so once Sheila gives us a green light.  

Images attached to this report
Comments related to this report
rahul.kumar@LIGO.ORG - 15:11, Tuesday 27 January 2026 (88920)

This afternoon Sheila and I went into the chamber and nudged some of the cables away from the OPO - Jeff will re-check the TF measurements to look for any improvements. 

There is a cable connector sitting on the OPO (which is a new addition to the OPO). I lifted that cable connector and then Sheila looked for alignment shifts - which she confirmed. For now we left the cable connector at the same spot on the OPO. We will think of moving it away after Jeff's results.

Sheila also found some changes in the beam alignment since last week - not sure if this is due to our work (AOSEM re-centered LHO alog 88910) from yesterday - although centering aosem-flag should not change the mechanical alignment. 

corey.gray@LIGO.ORG - 08:37, Wednesday 28 January 2026 (88938)EPO

EPO tagged

H1 SUS (SQZ, SUS)
jeffrey.kissel@LIGO.ORG - posted 10:48, Tuesday 27 January 2026 (88913)
H1SUSOPOS TFs post-OPO Crystal Swap / Translation Stage Improve -- Something Quite Off
J. Kissel, R. Kumar, B. Weaver, S. Dywer

Context
After the SQZ team felt done with OPOS suspension the re-install of the OPO (with an upgraded translation stage) we're following up on
    - Ryan's first look of the suspension's health (LHO:88851) 
    - After restoring the OPOS to normal control system configuration (LHO:88872) 
    - After recentering the AOSEMs (LHO:88910)

Measurement
I gathered more standard health check TFs. In doing so, I spruced up the excitation frequency response and data gathering templates to ensure good coherence. I also ran the TFs with all the damping loops besides the excitation degree of freedom ON to reduce incoherent motion from cross-coupling. The refreshed templates are 
    /ligo/svncommon/SusSVN/sus/trunk/OPOS/H1/OPO/SAGM1/Data
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_L_0p02to50Hz.xml
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_P_0p02to50Hz.xml
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_R_0p02to50Hz.xml
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_T_0p02to50Hz.xml
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_V_0p02to50Hz.xml
        2026-01-26_2054UTC_H1SUSOPO_M1_WhiteNoise_Y_0p02to50Hz.xml


Results
Attached is comparison of 
    - the opos dynamical model (Equations of Motion matrices: ssmake_voposus.m rev 12322; parameter set: oposopt_h1susopo_fit rev 12322)
    - the most recent, best at-vacuum, measurement of L1's OPOS
    - the last, best, at-vacuum measurement of H1's OPO prior to moving from HAM6 to HAM7
    - the last, bext, at-vacuum measurement of H1's OPO after moving to HAM7 (with a payload almost identical to what's installed now)
    - yesterday's measurement described above.

Focusing on page 6 first, one can clearly see that YAW to YAW transfer function is wildly different, implying a significant change to the dynamics of the suspension.
There's more supporting (but less signficant) evidence in 
    - pages 1 and 2 which shows and increase in the primary L / T resonance from 1.25 Hz to a split 1.32 Hz / 1.39 Hz
    - pages 1 thru 6 (all diagonal elements of the TF matrix) and pages 7 thru 20 (most off-diagonal elements) all showing a huge (tho incoherent) resonance in yaw at 4.98 Hz that was not there before
    - Nominally an oversight in the design, the expected large V to Y coupling looks quite impeded.

Discussion
After conversing with Sheila about what might have changed, or what might be impacting the dynamics, she reviews the changes:
    - The OPO cavity assembly (D1500296) has only a few changes -- the translation stage within is new, and there are now thin remote-control cables coming out of the assembly that weren't present before.
    - Those new remote control cables have been bundled into a pre-existing bundle, potentially making the system stiffer. We guess that this is the likely culprit of our problems.
    - Further the re-placement of the OPO assembly on the OPOS was not precise. It's plausible that the physical location of the cavity is now *slightly* different position, *potentially* changing the balance and mass ratio of how much moving mass is in which translational DOF. Maybe the source of L / T resonance shifts, but I doubt it. 

Also, conversing with Betsy and Rahul about the state of cables they found while centering the OSEMs:
    - They see a collection of cables (OSEM and SQZ) on the "far" (+Y) H3/V3 side of the OPOS that are resting on the platform without a good, dressed, soft connection between the platform and where the cable stress is relieved on the base.

Conclusion

We need to address / free-up the dynamics of this suspension before closing up the chamber.
Non-image files attached to this report
H1 IOO (ISC, OpsInfo, SEI)
jennifer.wright@LIGO.ORG - posted 10:42, Tuesday 27 January 2026 (88916)
Restored sliders on IMC SUS to December 3rd state

Jennie W, Jason O, Sheila D, Masayuki N,

 

Following Jim bringing HAM3 HEPI online (alog #88909) and isolating HAM3 ISI.

Jason and I restored the MC1, 2 and 3 sliders to their position on December 3rd during a lock when the mode-cleaner was locked with 2W input, HAM2 and 3 ISO Gain was , HAM2 and 3 ISI Guardian was set to 'isolated' and 2 and 3 HEPI guardian was set to 'RoBUST ISOLATED'.

This lock state for the IMC Guardian is 100. 

 

Before any adjustments today, we had 45 dB whitening gain on MC2 trans, and 91% of the power was in the 00 mode. This gave us 46 counts on MC2 trans nsum.

After HEPI, ISI, and suspensions are restored, we have mostly 10 mode, with 17.9 counts on MC2 trans sum, still 45 dB whitening gain.

I lowered the whitening gain to 30 dB to restore us to the normal whitening gain.

If we restore the alignment so that 90% of the power is in the 00 mode again, we should have 8.2 counts MC2 trans nsum

Images attached to this report
H1 ISC (INS, ISC)
keita.kawabe@LIGO.ORG - posted 18:07, Monday 26 January 2026 - last comment - 13:06, Tuesday 27 January 2026(88900)
JAC EOM Monday (Elenna, Keita, with remote help from Stephen, Michael, Matt and Gabriele)

Nothing wrong with our previous reflection dip measurements with alumina.

We (MichaelL, StephenA, MattH, Gabriele, Elenna and myself) had a meeting in the morning. 

Looking at the "with the alumina" reflection screen shots, Michael didn't see any serious problem so we decided that the electrode-crystal-face plate capacitance is OK. We won't worry about that, we'll just make sure that there's no visible gap.

Third mounting method ("in-between") was proposed and tested.

Stephen proposed an in-between method where we use washers between the input side plate and the front plate (bottom of three_methods.png cartoon). After the washer contacts the face plate AND the input side plate, screws are gently tightened in a balanced manner like in Appert method.  (In a retrospect this is not that different from Laxen method except the way screws are tightened and that the input side plate contacts with the face plate at two points.) 

We first tried to use a presicion thickness shim washer for 1/4-20 screws but I didn't like that they're too big. We ended up using smaller stamped washers that is 0.039" or 0.99mm thick (according to the caliper). That's not flat but seems OK to me.

This in-between method worked in that it was doable and gave us a reasonable reflection dips.

Mechanical stability test of Appert method and in-between method. The latter is better, we'll use that for the real RTP.

My original concern for the original Appert method (middle of three_methods.png cartoon) was that somehow the screw gets loose during transport or after a large change in the in-chamber temperature and the tuning will be off. Upon hearing this, Stephen proposed a test to loosen one screw and see if the tuning changes. We performed this test for both Stephen method and the in-between method. (Spoiler: yes.) We measured all four dip frequencies right after the alumina piece was mounted but only tracked the frequency change of 118MHz peak.

Loosening one screw changes the frequency, but the frequency change for the in-between method is an order of magnitude smaller (10 to 30kHz) than the original Appert method (300kHz) when the FWHM (or rather the width between the points where reflection is 6dB larger than the bottom of the dip) is about 70kHz or so. This is just one trial but I'm convinced that in-between method (or maybe Laxen method too though we haven't tried) is better, so that's what we'll do for the real crystal.

We only loosened the screws on the output side for both mounting methods. 

  Initial four frequencies Shaking? Loosen 1st screw Loosen 2nd screw
In-between method

9.142, 24.110, 45.972, somewhat

smaller than 118.214kHz

changed to 118.214kHz, unclear why.

(Something like 10k or 20kHz change,

couldn't cause another change by gentle tapping.)

118.214 -> 118.240

(+26kHz)

118.240 -> 118.251

(+11kHz)

Original Appert method 9.14685, 24.107, 46.066, 118.322

118.322 -> 118.592, caused by gentle tapping.

(+270kHz)

118.592 -> 118.876

(+284kHz)

118.876 -> noman's land

(>1MHz)

Shake and it will shift, we need to measure it again in chamber?

It's good to know that the in-between method can somewhat withstand the loosening of the second screw (because the tighter screws still support the face plate). However, it's disappointing to find that the assembly is susceptible to shaking.

In the in-between method, we couldn't record the initial 118MHz dip because it jumped up by 10kHz or so in front of our eyes when we were moving around the table. Not sure what happened but I assumed that it was some kind of shaking. However, I gently tapped the front and side plates and couldn't cause another shift.

In the original Appert method, since we knew something could happen, I tapped the front and side plates and there was a huge jump. See the difference between initial_118.jpg and taptap_118.jpg.

Even though we'll use in-between mounting method, it's plausible that the frequency shifts during transport or when the EOM lands on the ISI surface. I'm thinking we'll have to measure it in situ after everything is tuned in the lab.

What's to come tomorrow.

We'll install RTP and tune. Before doing that, though, I'll discuss inserting indium foil between the crystal and the front plate with Masayuki. Michael suggested that (and even between the crystal and the electrode, though that would be tricky) today, Masayuki and I talked about the possibility briefly last week, it just sounds like a good thing as a buffer to absorb gaps here and there.

Other things.

In the previous alog (88886) in one of the pictures (gap.jpg), there was a time when it looked as if the circuit board was slightly bowed. We took a picture of the electrode today (electrode_contactpoint.jpg) and it looks as if the electrode is more abraded close to the outside edge of the crystal, so maybe the board bowing is real.

 

 

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keita.kawabe@LIGO.ORG - 13:06, Tuesday 27 January 2026 (88918)

Why (change in) the gap might matter.

Gabrilele asked me why a tiny gap matters so I made a quick calculation.

Suppose that we can ignore the edge effect at the edge of the electrode for convenience, we can replace the 4x4x40mm crystal with an infinitely wide and long crystal that is 4mm thick, and replace the capacitance with the capacitance per area.

In the attached, the electrode, the crystal and the face plate are all inifnitely larger in a plane orthogonal to the surface of my log book. Thickness of the crystal is d (4mm). There's a gap of delta between the electrode and the crystal, and there's no gap between the crystal and the face plate (but it's not important where exactly the gap is).

Under such a configuration, if you do the math, the capacitance per area is equal to the no-gap capacitance per area multiplied by 1/(1+epsilon*delta/epsilon_0/d) where epsilon and epsilon_0 are the permittivity of the alumina and vacuum, respectively, and the former is 10 times the latter.

In the end, the capacitance with the gap is a factor of

1/(1+10*delta/4mm)

smaller than without the gap.

The capacitance with a 0.1mm gap is 80% of that without the gap, 0.2mm and it's 67%, 0.3mm (12 thou) and it's 57%. If the gap doesn't change, maybe that's OK. If the gap changes it will change the tuning via capacitance change. There are other effects (like coil winding) but the capacitance change via the gap change cannot be ignored/dismissed.

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H1 TCS
sophie.muusse@LIGO.ORG - posted 18:04, Monday 26 January 2026 - last comment - 10:48, Tuesday 27 January 2026(88902)
CHETA Progress - second table

S Muusse, M. Todd


New QCL unit (0920) has been put in place of original unit (0923) which is malfunctioning (cause unknown). Initial profiling has taken place and L1 focal length is 10% larger than spec.


QCL unit failure summary:

All day on 2026-01-21 we were running the laser at 900mA doing beam profiles and alignment work. No malfunctioning was witnessed and the laser unit was operating as expected, similar to the laser unit we had run in December for a week. Before lasing we set the following limits on the LD and TEC, per the datasheet.

  1. LD current limit was set to 1.05A
  2. LD voltage limit was set to 12.9V
  3. TEC operating temperature was set to 20C

On 2026-01-22 we turned the laser on to do some more beam profiling with the same limit settings as yesterday, but setting the LD current to 1A (forward voltage was around 12.2V) as was done when we originally profiled this laser in September. We were in the middle of setting up for a new beam profiling measurement (alignment showed the beam was fine, as usual) and we blocked the beam with a high power beam dump at the laser head while installing the profiler. Upon removing the beam dump, we noticed no power was coming out of the laser, and then noticed the forward voltage had dropped to around 800mV. We noticed no sounds or smells or any other signs that something had stopped, only sudden lack of light coming from the unit. All other settings were fine, meaning the controller had not faulted and was still outputing 1A LD current and the TEC was maintaining 20C.

We ran the following checks to see if we could remedy the problem, without success.

  1. Checked the cable connection to the laser unit (pins on the laser unit looked fine)
  2. Checked the Laser Controller cable connections (pins in the DSUB connectors looked fine)
  3. We tried a completely new laser controller box and new cable. The settings were similarly set and the same behavior was seen with the forward voltage response to the LD current setpoint.
  4. We tried changing the TEC setpoint to be 25C, and the same behavior was seen with the forward voltage response to the LD current setpoint, and failing to lase as usual.
  5. We used the same cable and laser controller on the previous QCL unit, and it operated as expected --- lasing fine as usua

QCL 0920 profiling summary:

Replaced broken unit with 0920 and confirms it lases as spec'd. We built telescope as modelled but beam profile was 75% of expected beam width at L2. We subsequently profiled the laser output and confirmed QCL output q measured previously by Matt was still correct. We became suspicious of the true focal length of L1. Then we profiled multiple places after L1 and fit a q parameter using a non-linear fit. A plot of this fit is attached. Using these 2 q parameters the focal length of L1 was estimated to be 220mm instead of 200mm as spec. We think this is mostly because L1 focal length stated by manufactorer is for 588nm where the refractive index is almost 3% larger than at 4.6um. Focal length in the model was modified to reflect our estimated f1 which predicted a beam size closer that measured earlier. 
Side note: the scanning slit beam profiler reflects significant amount of 4.6um light which is observable on a thermal beam card. 

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matthewrichard.todd@LIGO.ORG - 10:48, Tuesday 27 January 2026 (88914)

This morning we continued profiling to characterize the true L2 focal length and install the modeled telescope and characterize it.

We replaced L1 with L2 in the telescope and made several measurements to fit for a q-parameter after L2, because we think we know the q going into it quite well. Then with the q parameters, you can estimate the focal length using ABCD matrix for a thin lens (our estimates yield relatively low complex angles, less than 1 deg, making confident estimates).

Parameter x [m] y [m]
Input q (coming from the laser) 0.411 + 0.067i 0.376 + 0.056i
Output q (fit from profiles) 1.496 + 1.289i 1.221 + 0.632j
Focal Length (-q1/(q1/q2 - 1) 0.503 0.511

Average focal length of L2 = 0.507 m. Which is around 1.5% different from the spec'd value. To reiterate Sophie's log above, the focal length of L1 is estimated to be 0.217 m. Which is almost 9% different than the spec'd value. With these values in hand (as well as the updated value for CaF2 refractive index at 4.6um), we can make a more accurate model and see if measurements of the outgoing q-parameter from the telescope match that model.

We installed a telescope as set up in a model and measured several proviles to fit for the q-parameter after L2. The modeled waist size in both the horizontal and vertical are within the fit uncertainty; however the waist position of the modeled beam is roughly 20cm off in both directions. I think this is because of the Gouy phase regime that we are sampling gives better estimates of the waist size and since we did not sample near the waist we do not have a good idea of where it is.

This afternoon we will try and re-build the telescope as optimized in our models with these measurements to see if we can get a q-parameter that will be 53mm at the "ITM" (propagated 35m from L2).

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H1 IOO (IOO)
rahul.kumar@LIGO.ORG - posted 13:04, Wednesday 21 January 2026 - last comment - 09:41, Wednesday 28 January 2026(88834)
HAM1 update - JAC damper

Jason. JennieW, Rahul

This morning we added the damper parts to the JAC in HAM1 chamber - see picture attached. The cables were re-routed slightly so that they don't interfere with the damper.

I have finger tightened the screws of the damper for now - since no torque spec was provided and we were worried that tightening them too much might affect its position/angle.

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corey.gray@LIGO.ORG - 08:27, Wednesday 28 January 2026 (88934)EPO

EPO-tagged.

jason.oberling@LIGO.ORG - 09:41, Wednesday 28 January 2026 (88941)

Masayuki and I fully tightened the JAC body mode dampers yesterday.  We were only able to get the screws ~1/2 turn past finger-tight before we could no longer tighten them.  No changes in JAC alignment were observed while we were doing this.

H1 SUS (SUS)
ryan.crouch@LIGO.ORG - posted 11:44, Wednesday 21 January 2026 - last comment - 08:25, Wednesday 28 January 2026(88828)
2nd HXDS received from LLO

Yesterday I picked up the shipment from LLO contain the 2nd HXDS (first HXDS shipment alog87998) and related ASSEYs and brought it to the Triples lab. 

Uwrapping and inspecting was uneventful, the zip ties were intact, the shock pads untripped and the humidity indicator was unchanged in color. The outer (front, back) and inner (front, back) bags were in good condition, unwrapping the suspension I found no play with the blades.  All the nuts and dowel pins were tight and well seated, the ICS looks good except for it seems to be missing the HDS Intermediate Mass Fixture (D2000230-V1, s/n 08). The part is scribed as V1, on the dcc there's a V2 with two added 8-32 helicoils taps that, based on D1900352 which uses V2, I should be able to see from the front and I don't, so this is a V1 plate and not an incorrectly scribed V2. I believe these two missing 8-32 holes are where we will attach the BOSEM Mounting plate (D2000257). The first HXDS we received in November had the V2 plate. We may have to do a small rework to update it to V2, or have LLO send the V2 part if possible.

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corey.gray@LIGO.ORG - 08:25, Wednesday 28 January 2026 (88933)EPO

EPO tagging

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