TITLE: 09/10 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Commissioning
INCOMING OPERATOR: None
SHIFT SUMMARY:
The Mega Clean room was Turnt Off. For What!? You may ask? Because we are trying to get closer to our final LVEA temperature for locking the IFO.
GRB-Short E646174 notification @ 1:24:41 UTC
H1 is now sitting in down er rather Prep for locking..
LOG:
| Start Time | System | Name | Location | Lazer_Haz | Task | Time End |
|---|---|---|---|---|---|---|
| 22:35 | vac | VACteam | EY | - | vendor visit to EY | 23:50 |
| 23:42 | VAC | Jordan Gerardo | LVEA HAM7 | N | Valving swap on HAM7 | 23:53 |
| 00:40 | VAC | Gerardo | LVEA | N | Turning Off the Mega Clean room | 00:49 |
Sheila, Elenna, Jenne
Morning locking notes
At this time we held in down to allow relay tube work, and used the time to measure the oplev damping and try switching to using M3 wit for lower stage damping instead.
I measured the oplev damping OLGs, pitch and yaw. The reference traces use the oplev as the sensor for the damping, and the live traces use the M3 wit as the sensor but a different matrix value that Sheila calculated based on this alog.
We then switched to M2 damping using M3 wits as the sensor, and compared the BS spectra with no lower stage damping, oplev damping, and wit damping, comparison here. We see good suppression of the modes and less sensor noise injection on the M3 wits.
Here is a screenshot of the "OLDAMP" settings we want to use on M2. I want to clarify that even though we are now using the M3 wits as the sensor, the damping is still running through the oplev damping bank on M2.
At this point, we decided to break further and allow Filiberto to update the resistors on the M1 QOSEMs, so our lockloss transient from saturation is reduced.
***
After Fil and Oli finished the sat amp changes, we began locking again. We locked PRMI with M3 wit damping engaged before the triggering occurred so there was no lockloss. Once locked, the guardian disengages the lower stage damping.
Sheila measured the BS motion using oplev and M3 wit without the L2P decoupling engaged but the wit damping off. She checked the MICH and PRCL OLGs and we saw that they were fine. MICH UGF is 8.5 Hz, PRCL is 60 Hz.
I engaged the L2P decoupling, and we saw that low frequency pitch motion was reduced. However, there was still a large 0.45 Hz peak. With the M3 wit damping reengaged, the peak is reduced. See plot
Recipe for successful PRMI: M3 wit damping engaged, L2P decoupling engaged. Once we can reengage MICH ASC, we can turn off the M3 wit damping. I have SDFed the filters for BBSS M2 L2P decoupling 1 2
There is a lot of alignment drift in BS yaw while we sit locked. I had to touch up the aligment by hand.
We stayed in PRMI for 25 minutes.
***
We struggled to lock DRMI, and eventually chose to relock PRMI and fix the alignment. After this, DRMI locked quickly. We lost lock at the 3 f transition, so Sheila went to check we were aligned to REFLAIR 3f diodes. Then, I rephased the diodes while locked in PRMI by injecting a PRCL line and maximizing the height in 27 I, and a MICH line to maximize the height in 135 Q. PRCL, MICH, SDF
With DRMI locked, we saw that the PRCL OLG looked strange, so I also checked the REFLAIR 1f phasing. I made a minimal change to reflair 9 to improve PRCL in I and a 50 deg change in 45 to reduce SRCL in 45 Q. PRCL, SRCL, SDF
Sheila's guardian changes, to improve some problems we faced when locking.
***
Jenne and I attempted to check the PRCL/SRCL decoupling in the LSC matrix, and measured a value by injecting a PRCL line into reflair 9 and 45. However, the resulting OLGs looked even worse. Both PRCL and MICH look very strange, possibly indicating cross coupling. Unfortunately I don't have images of the PRCL transfer function but here is the MICH tf.
Seems like the phasing is wrong, but the loops became more unstable when we reverted the phasing changes I made earlier.
[Gabriele, Jenne]
Gabriele pointed out that the funny MICH OLG almost looks like a strange situation with the BBSS crossover. We tried changing the H1:SUS-BS_M3_DRIVEALIGN_L2L_GAIN from nominal 1, to 0.5 and also 2. This changed the high frequency part of the MICH OLG, but never made it 'better'.
I tried measuring the BBSS M2/M3 crossover, using a template I found in Elenna's directory that looks like it's from alog 91713. Her references from no-arm MICH-only are the green squares. The nominal (gains of 1 everywhere) measurement with DRMI locked (arms off resonance) is red circles. I don't think it makes sense to me why the crossover is so very different right now. I tried changing H1:SUS-BS_M3_DRIVEALIGN_L2L_GAIN as well as H1:SUS-BS_M2_DRIVEALIGN_L2L_GAIN, but never could get the crossover to look like anything sensible.
So, on the one hand, we still don't know why the DRMI OLGs are so weird, but on the other hand we can stay locked with DRMI for ~infinity minutes, as long as we touch up the alignment every 20 minutes or so.
I'm leaving the IFO requested to DOWN, so that when the DRMI finally drifts too much, it won't try to relock until a person is here to watch it.
TITLE: 09/09 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Commissioning
OUTGOING OPERATOR: Corey
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 16mph Gusts, 9mph 3min avg
Primary useism: 0.02 μm/s
Secondary useism: 0.11 μm/s
QUICK SUMMARY:
The Comissioners are Working on DRMI alignment and Locking seems like H1 is going through Green Arms and IR just fine.
VAC Team is currently working on HAM7 valving.
TITLE: 09/09 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Commissioning
INCOMING OPERATOR: Tony
SHIFT SUMMARY:
H1 Commissioning continued with relatively stable PRMI locks + 2-DRMI locks, and continued locking work (i.e. alignment tweaks, Length to Pit decoupling measurements, BS satamp whitening change, rfpd phasing, checking pointing on REFL A/B)
Relay Tube install started late morning with disassembly on HAM5 and then pumping down the Relay Tube (Gate Valves on both sides of the Relay Tube will remain CLOSED). Relay Tube leak checked (no leaks observed, VAC will turn OFF Mega-cleanroom at end of day)
BBSS had a satamp change to address
LOG:
I tried to repeat Masayuki's measurement in this alog to calibrate the JM3, MC1, MC2 and MC3 angular motion into uradians using the IMC cavity transmission, see this alog #91487.
This injects a line in turn on each steering mirror in pitch and yaw and looks for the height of the second harmonic of this line in the IMC transmitted power, as this should depend only on the size of the dither we apply to the alignment and not any existing static mis-alignment.
First I paused the IMC lock guardian and then turned off the IMC WFS (take gain to 0).
I then injected a line on JM3 pitch, then JM3 yaw. There were both at 30 counts into H1:SUS-JM3_M1_TEST_P_EXC and H1:SUS-JM3_M1_TEST_Y_EXC respectively.
The 2f line is viisble at 22 Hz as seen in the transmitted power ASD for the pitch excitation and the yaw excitation.
I then tried to do the same for MC1. I used 17Hz as my dither frequency and checked this didn't overlap with any modes of the MC1 mirror by checking the DAMP filter bank.
I could not get good measurement coherence at 34Hz with a 30 count excitation, when I went up to 60 counts the cavity unlocked, so I turned off the excitation, unpaused the guardian and brought the mode cleaner to down.
This plot shows the ASD during the 30 count injection with the red lines marking the 1f and 2f lines.
Looking back at the ndscope for the time when I thought the IMC unlocked (the mc trans camera spot flashed), it looks like the cavity did not unlock completely but started oscillating at 1Hz.
The first cursor is when the cavity lock started oscillating and the transmitted signal on IMC-TRANS PD went from 11000 counts to 6700 counts. When I turned off the excitation it went back up to the locked level again.
Second cursor is where I purposely brought the mode cleaner to down and the IMC TRANS PD went to 4000 counts.
Summary: I can use a dither on JM3 to measure the calibration of this mirror but to measure the MC mirrors I need to tune my excitation more precisely.
Fil, Oli
Fil went ahead and did another modification to the BBSS M1 QOSEM satamp. This is the same modification that LLO had done (LLO:82137) - on each of the six boards, resistors R902, R1002, R1102, R903, R1003, and R1103 were swapped from 499kOhm to 22kOhm resistors.
Before the modification the satamp whitening was zpk([0.0144],[2.89],1), with compensation filter zpk([2.89],[0.0144],1). Changing these resistors has shifted the whitening zero up in frequency so the satamp whitening is now zpk([0.263],[2.89],1), with the new compensation filter zpk([2.89],[0.263],1). I have updated the whitening compensation filters ( BS_M1_OSEMINF_{F1,F2,F3,LF,RT,SD}_{SUM,X_RAW,Y_RAW} ) in OSEMINF to these new compensation filters.
Before we brought the BBSS back up we noticed that the SUM counts for F1 were railed, and that the SUMs for all other osems were between 18-20k counts. This is with the sum feedback on. When we turned the sum feedback off and just sent a constant current to the LEDs, F1 was still railed, but the other osems all jumped to normal varying SUM values that we had seen months ago prior to turning the sum feedback on - F3 and RT were staturating (like they had been doing back then), and the others were around 30k counts. Switching back to the sum feedback mode, we have been seeing the SUM counts all (except F1) climbing up slowly, and will hopefully stop in their nominal feedback on locations. We aren't sure why F1 is showing the counts as saturated though while in sum feedback mode - it hadn't been saturated before, and either way, turning on sum feedback mode should lower the current to the LED to lower the counts to a reasonable level (between 29k and 30k counts).
PSL Status Report - Weekly FAMIS 64006
Laser Status:
NPRO output power is 1.86W
AMP1 output power is 70.67W
AMP2 output power is 139.5W
NPRO watchdog is GREEN
AMP1 watchdog is GREEN
AMP2 watchdog is GREEN
PDWD watchdog is GREEN
PMC:
It has been locked 14 days, 3 hr 2 minutes
Reflected power = 28.44W
Transmitted power = 104.6W
PowerSum = 133.0W
FSS:
It has been locked for 0 days 0 hr and 18 min
TPD[V] = 0.4517V
ISS:
The diffracted power is around 4.4%
Last saturation event was 0 days 4 hours and 22 minutes ago
Possible Issues:
PMC reflected power is high
JAC REFL beam seems to be flickering in the video because the 809Hz length dither frequency is close to the integer multiple of the video refresh rate. I disabled the 809Hz length dither momentarily and the flickering was gone, see the attached video.
If we can see the effect of the dither just by using the video like this, the length dither amplitude is probably too large to enable in observing. One omega peak observed by ISS array is huge.
For FAMIS #62540: All fan trends look fairly flat (even after the step-down 5-days ago which Tony notes in alog 91811).
This is for FAMIS #64007.
Laser Status:
NPRO output power is 1.846W
AMP1 output power is 70.55W
AMP2 output power is 139.4W
NPRO watchdog is GREEN
AMP1 watchdog is GREEN
AMP2 watchdog is GREEN
PDWD watchdog is GREEN
PMC:
It has been locked 13 days, 21 hr 33 minutes
Reflected power = 28.32W
Transmitted power = 104.6W
PowerSum = 132.9W
FSS:
It has been locked for 0 days 9 hr and 2 min
TPD[V] = 0.4572V
ISS:
The diffracted power is around 4.3%
Last saturation event was 0 days 9 hours and 52 minutes ago
Possible Issues:
PMC reflected power is high
TITLE: 09/09 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Commissioning
OUTGOING OPERATOR: None
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 5mph Gusts, 2mph 3min avg
Primary useism: 0.01 μm/s
Secondary useism: 0.13 μm/s
QUICK SUMMARY:
Looks like great progress yesterday with X-arm opened and locking green arms. This morning ISC LOCK is at Prep For Locking, there were multiple dust alarms, and all is fairly quiet otherwise.
Reran launch script for nuc25 to bring up the DRMI FOM Displacements dtt.
Camilla, Ryan S, Louis, TJ, Elenna
After GV20 was opened, we were able to successfully lock the X arm on green and send both slow control and green WFS control to ETMX!
We have rerun the baffle scripts for TMSX, ITMX, TMSY and ITMY. We have locked both arms on green, ran the green wfs, and ran through ETM_TMS_WFS_OFFLOADED. Then, we used these positions of the ITMs to set the green camera offsets. This means we can now full run the green arms initial alignment state, and no longer need to run baffle pd scripts to position the ITMs.
Camilla, TJ, Ryan and Louis worked to run the baffle scripts. They had some difficulties with ITMY because it seems to have started in a weird place, but Camilla moved ITMY around by hand enough that she was able to get the script to run properly.
From there, locking the green arms was straightforward, and there were no issues. I've attached the SDF screenshots of the new green camera offsets.
Reminder of how to do this:
I set the flags in lscparams, gate_valve_flag = False, and no_ETMX_actuation to False.
ALS COMM and DIFF locked without any issue (except some guardian typos we introduced with our new flag), and I stepped manually through some initial alignment steps manually adjusting alignments and usuaing the guardian to lock cavities.
The AS 45 error signal for MICH dark didn't look right, this was because ETMY test offsets were off, even though the guardian state said it was misaligned. There was a message on the suspension overview screen saying test offsets are off. I'm not sure why this happened, or if we can make the way the guardian handles this less confusing. X arm IR, PRX, SRY had no issues.
Locked ALS again, COMM had to do the full search to find IR, I updated the last value in the list with the found location.
In PRMI POP18 flashes up to 150 counts, (I_ERR_DQ channel). I accidentally kicked the BS when I added a yaw element to the new BS damping matrix we added this morning (91834).
PRMI did not lock quickly, we may need to undo some of the changes in 91530 and 91501 now that we have the arms back.
Sheila suggested we adjust the top mass damping to improve the step response, 91808. I created a 20 Hz elliptical low pass so we could raise the gain even further. However, this has little effect on the 0.45 Hz ringing in the step response, because this is not coming from the top mass. This is evident in the OLTFs, see pitch below. There could be cross coupling with length, but more likely this is some pitch mode between the lower stages that is not witnessed in the top mass osems. Therefore, damping it will have to occur with a lower stage damping loop using the oplev or M3 wit.
As it stands, we're getting plenty of suppression in LPY with the top mass damping. With the updated model, 91834, we can revisit lower stage damping.
***
I wanted to add some details about a challenge we are having with the beamsplitter. In short, if the BBSS is kicked a large amount, this saturates the QOSEMs to the point that the top mass damping loops cannot be used, and we have to put the beamsplitter in safe until the suspension freely damps enough that we can reengage damping.
This happened four times today, and has happened at least twice before. The first time occured today because I was adjusting damping gains and put a gain that was so large it rung up the loop. It took about 10-15 minutes to damp down. This kick also trips the ISI.
The other three times occurred today while we were trying to lock MICH dark during initial alignment. I had put the beamsplitter into what I thought was a decent enough alignment to lock MICH dark- clearly it was not because the MICH loop engagement kicked the beamsplitter significantly. I tried twice more after touching up the alignment further and the same problem occurred. From a quick glance, it looks like the MICH and BS lock settings were correct, but I with carefully check tomorrow one more time before we try this again.
Sheila notes that the big kicks in MICH dark were because although ETMY was marked as "misaligned" by the guardian, it was not actually misaligned, 91842. So that mystery is solved. We still need to come up with a strategy to handle the times the beamsplitter does get kicked, though.
WP13584,13585 Add 7th ADC to h1oaf0 IO Chassis, add to models
Erik, EJ, Jonathan, Fil, Dave:
A 7th ADC was added to h1oaf0's IO Chassis. Because all the cards in this chassis had been shifted left by one slot to move the 20bit-DAC from A1-4 to A2-1, there was only one slot ADC6 could go into, A3-4.
Erik and EJ took the opportunity of powering h1oaf0 to check the BIOS settings (some needed changing), performing Adnaco benchmark tests, and disconnecting A4 from the computer.
Fil installed the new AA chassis for ADC6, it currently does not have anything connected to its inputs.
Dave made h1iopoaf0 and h1pemcs model changes. PEM reads out all 32 channels of ADC6 into filtermodules H1:PEM-CS_ADC_6_[0-31]. These FMs have been turned on.
DAQ restart was required for the model changes.
WP13591 h1susbs add M3 matrix
Sheila, Ellena, Dave
A new h1susbs model was installed. A DAQ restart was required
WP13592 h1crsproc add BLRMS
Jim, Erik, EJ, Dave
A new h1crsproc model was installed. A DAQ restart was required
Note that the svn server redoubt was not available for a rev-lock build, so we did a "old fashioned" install
> rtcds build h1crsproc
> INSTALL_ONLY_REV_LOCKED=false rtcds install h1crsproc
DAQ Restart
Jonathan, Dave:
After the round of model restarts the DAQ was restarted; 0-leg followed by 1-leg. No EDC restart was required.
All framewriters rode through the restarts with no issues.
BIOS setting changed, now matching the LIGO-T1300430 document:
CPU C State Control :
Enhanced Halt State (C1E) : Enabled -> Disabled
Package C State Control:
Package C State : Auto -> C0/C1 state
We noted that h1oaf0's 6th ADC (ADC5) had failed its AUTOCAL. Trending shows this has been the case for at least 9 months.
J. Kissel, J. Wright
Jennie and Marc did some dark noise investigations yesterday afternoon, found grounding issues, but then reverted the temporary configuration that improved the situation.
However, this morning, mis-reading their aLOG thinking that the solution was still in place, I re-took new ASDs excited to see QPDA fixed.
Even though their temporary solution has been reverted, QPDA still seems to be fixed.
So -- here's some excellent, final answer plots for pitch and yaw, comparing HAM2 and HAM3 rotation against their local sensors.
PITCH
- Now, as expected, the whitened ADC noise QPDA aka ISIK's HAM3 sensor is the factor of ~5x larger where the QPD is limited by ADC noise above 0.5 Hz, and it has the same inverse-whitening-filter shape as QPDB.
- Encouragingly, the QPDA ISIK optical lever PIT signal matches the HAM3 CRS RY signal below 0.5 Hz -- so this QPD will be at least a little bit useful!
- The noise floor of the QPDA ISIK optical lever PIT signal is better than the CRS above ~2 Hz, though the actual platform motion (as reported by the GS13s) is still much lower than that.
Very interesting science --
- The improvement in platform motion of HAM3 from blending in the CRS is corroborated with the ISIK optical lever signal below 0.5 Hz.
- The QPDB measure of HAM2 shows that there's a lot more physical motion in PIT in the 1 to 10 Hz region than is reported by the in-loop GS13s. In that region, the QPD's signal is a factor of 10 above the noise floor, so I'm pretty sure this is real signal.
YAW
- Again, the two SPI QPDs noise floor now makes sense, with the QPDB (on HAM3) measurement of HAM2 (ISIJ) noise floor being a factor of ~5x better than the QPDA (on HAM2) measurement of HAM3 (ISIK).
- Thus, the SPI OL YAW measure of HAM2 agrees with the local HAM2 sensors up to ~0.8 Hz, but the OL YAW measure of HAM3 only agrees up to 0.5 Hz.
Measurement time: 2026-09-04 16:47 UTC. I took 25 averages with a 0.01 Hz frequency resolution. Hanning window with 50% overlap.
ISIs were isolated, IMC was locked, still no IFO tho. sensor correction was ON in the nominal WINDY configuration. No earthquakes. CRS is blended in with ISI HAM3.
Spots centered, nominal sum voltage.
DTT Calibration of traces beyond what's done in the front-end is what's quoted in LHO:91809, namely -- just a conversion of nanoradians to radians for sensors already in displacement, and converting the GS13s from inertial sensor units asymptoting to 1 [nm/s] into displacement by inverting the ideal 1 Hz pendulum response.
Summary: The excess noise on the ground for both QPDA and B seems to come and go.
I re-measured the dark current on QPD A and B to figure out why Jeff's measurements show that the QPD A spectrum no longer looks wrong. Following the prcoedure we followed for the dark noise measurement of the QPDs in LHO alog #91772.
I shuttered the SPI laser and put an offset of 11000 on QPDA and 12400 on QPD B to give a fake signals on each quadrant that matches the voltage on each QPD when the laser is unshuttered.
Then I measured an ASD of all 8 QPD quadrants. There was a glitch so I switched to doing an accumulative measaurement. You can see that both QPDs have some noisier quadrants.
I also took a time series and right before started the measurement above you can see a glitch in the level of each quadrant.
Marc and I are going to do more ground loop checks. After talking with Jeff each QPD is meant to use the TIA ground (rack ground) as a reference but if there is some grounding problem in the chamber at the QPD itself maybe we are getting some intermittent signal pick-up on this ground loop.
Marc and I checked QPD B and this is also grounded to chamber ground through pin 13. Each other pin is isolated. We confirmed pin 13 is also connected to the chassis ground.
We did not check the third TIA chassis (variant 3) as this gets its input signals from TIA chassis 2.
New plots with noise models.
I wanted to get a rough number for the JAC error signal in Hz, this it to allow Jeff and I to measure the frequency noise of the JAC as an independent monitor of the IMC frequency noise which will allow us to compare the IMC length noise to the SPI length noise.
I think Masayuki calculated this back in March LHO alog #89399 but I wanted to recheck it as the Guardian settings have been changed since then.
I measured the unlocked error signal Vpp at H1:JAC-L_SERVO_IN1_DQ to be 1.01365V.
The value in metres is the half-width at half-maximum of the cavity.
First calculate the HWHM in Hz:
HWHM = FSR/2*Finesse = 0.595 MHz.
The finesse was measured by Masdayuki and I at Caltech for our JAC which is unit 008 (see E2500324).
The FSR of the JAC I got from T0900616 to be 148.5MHz (couldn't find the exact FSR for this specific unit mentioned anywhere so used the one quoted in the PMC design document).
This means to measure the frequency noise we need to multiply the signal at
H1:JAC-L_SERVO_IN1_DQ by 0.587 e6Hz/V to measure frequency noise.
After discussing with Masayuki he reminded me that the JAC is less stable a reference than the IMC as it is not a suspended cavity. So we should use the IMC length noise as our SPI reference.
After the angle calibrations were applied to the SPI readout channels, I grabbed some data to check whether the SPI is roughly agreeing with the ISI sensors. I used the supersensor OUT channels for the ISI sensors (these are the signals behind the blending filters, before the summation for the blended supersensor). Screenshots from diaggui are attached.
For the differential X degree of freedom (SPI length), the visual agreement is remarkably good.
The optical lever (angle) measurements are harder to interpret. First of all, QPD A has an as-yet-unresolved noise issue, which Jennie is currently investigating. Aside from this, the results look very encouraging, since the CPS and GS13 at least somewhat agree with the SPI.
These spectra should be regarded as a first result, but not yet final. We will post a better analysis once the error has been resolved.
Note: If anyone has suggestions for which sensor channels would provide a better/more appropriate comparison than the supersensor OUT channels used here, please comment, your input is welcome.
Brian pointed me to a set of new data channels that provide calibrated outputs directly in displacement units. Using these channels, I acquired spectra with DTT at UTC 2026-09-09 12:00:00 (BW = 0.01 Hz, 30 averages) and generated the plots that follow
Channels plotted — Angular (RY / Pitch):
Optical lever pitch signals (angular, rad/√Hz):
H1:SPI-H23_OL_ISI_J_PIT_OUT_DQ (ISI 2) — Optical lever ISI J pitch angleH1:SPI-H23_OL_ISI_K_PIT_OUT_DQ (ISI 3) — Optical lever ISI K pitch angleISI blend / CPS RY signals (ISI RY witness channels):
H1:ISI-HAM2_BLND_CPSRY_IN1_DQ (ISI 2) — HAM2 blended CPS RY inputH1:ISI-HAM3_BLND_CPSRY_IN1_DQ (ISI 3) — HAM3 blended CPS RY inputISI calibrated Cartesian RY signals (rad/√Hz):
H1:ISI-HAM2_CAL_CART_RY_OUT_DQ (ISI 2) — HAM2 calibrated Cartesian RY outputH1:ISI-HAM3_CAL_CART_RY_OUT_DQ (ISI 3) — HAM3 calibrated Cartesian RY outputDifferential Z displacement channel (converted to rad/√Hz):
H1:ISI-DIFF_H23_SS_Z_OUT_DQ — Differential H23 SS_Z displacement. Given in nm/√Hz; converted to m/√Hz, then divided by the arm length (15.4 m) to yield rad/√Hz.Channels plotted — Differential X motion (displacement):
H1:SPI-H23_DIFFDISP_MAIN_OUT_DQ — SPI H23 main differential displacementH1:ISI-DIFF_H23_SS_X_OUT_DQ — Differential H23 SS_X (CPS + GS13 supersensor)H1:ISI-HAM2_BLND_CPSX_IN1_DQ (ISI 2) — HAM2 blended CPS X inputH1:ISI-HAM3_BLND_CPSX_IN1_DQ (ISI 3) — HAM3 blended CPS X inputH1:ISI-HAM2_CAL_CART_X_OUT_DQ (ISI 2) — HAM2 calibrated Cartesian X output (GS13)H1:ISI-HAM3_CAL_CART_X_OUT_DQ (ISI 3) — HAM3 calibrated Cartesian X output (GS13)All scaled by nm_to_m (nm/√Hz → m/√Hz).
Unit conversions: