TITLE: 03/25 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Preventive Maintenance
INCOMING OPERATOR: Oli
SHIFT SUMMARY: Busy maintenance day mostly focused on preparing cabling for HAM1 ISI installation. After that wrapped up, ran an initial alignment with some code testing, then H1 was able to lock without issue and fully automatically. Had to wait in OMC_WHITENING to damp violins (likely my fault for breaking lock during powerup this morning).
LOG:
Start Time | System | Name | Location | Lazer_Haz | Task | Time End |
---|---|---|---|---|---|---|
14:38 | FAC | Kim | EX | N | Technical cleaning | 16:04 |
14:49 | FAC | Chris | X-arm | N | Tumbleweed clearing | 19:58 |
14:58 | CAL | Tony, Francisco | PCalLab | Local | Prep for measurements | 15:28 |
15:00 | FAC | Tyler | Staging | N | Moving ISI container; shop -> staging | 15:43 |
15:11 | CDS | Erik | CR | N | Rebooting FOMs | 15:11 |
14:38 | FAC | Nellie | EY | N | Technical cleaning | 15:17 |
15:27 | IAS | Jason, RyanC | LVEA | N | FARO surveying | 19:14 |
15:29 | CAL | Tony, Matt, Francisco | EX | YES | PCal measurements | 17:58 |
15:34 | AOS | Camilla | LVEA/OptLab | N | Putting away parts | 15:59 |
15:36 | CDS | Fil, Marc | LVEA/CER | N | HAM1 field cabling | 19:25 |
15:43 | VAC | Travis, Janos | EX | N | Compressor work | 18:25 |
15:44 | FAC | Tyler | CS/MX/MY | N | 3IFO and capital inventory | 19:44 |
15:46 | VAC | Richard | LVEA | N | Turn on roughing pump panel | 17:07 |
15:59 | VAC | Jordan, Janos | LVEA | N | Bringing parts in via FC door | 17:07 |
15:59 | FAC | Tyler, Contractor | H2 Building | N | HVAC work | 19:59 |
16:02 | FAC | Mitchell | LVEA | N | Clearing off SEI racks | 17:12 |
16:05 | FAC | Kim | LVEA | N | Technical cleaning | 18:54 |
16:08 | AOS | Betsy | LVEA | N | Checking on progress | 16:25 |
16:14 | SEI | Jim | LVEA | N | Checking on progress | 17:12 |
16:19 | TCS | Camilla | OptLab | N | Grabbing parts | 16:23 |
16:21 | ISC | Mayank, Jennie | OptLab | Local | ISS array work | 20:52 |
18:12 | SEI | Jim | LVEA | N | Testing loadcell readers | 18:27 |
19:15 | CDS | Richard | LVEA | N | Talking to Fil and Marc | 19:21 |
19:17 | AOS | Jason | OptLab | - | Inventory | 19:28 |
19:30 | OPS | Camilla | LVEA | N | Sweep | 19:45 |
20:36 | CDS | Marc | CER | N | Listening for power supplies | 21:07 |
20:54 | ISC | Keita, Mayank | OptLab | Local | ISS array work | 22:45 |
21:22 | TCS | Camilla, Matt | OptLab | Local | CO2 laser work | 22:30 |
TITLE: 03/25 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Preventive Maintenance
OUTGOING OPERATOR: Ryan S
CURRENT ENVIRONMENT:
SEI_ENV state: SEISMON_ALERT
Wind: 3mph Gusts, 1mph 3min avg
Primary useism: 0.02 μm/s
Secondary useism: 0.25 μm/s
QUICK SUMMARY:
Waiting in OMC_WHITENING still while damping violins. We're pretty close so hopefully will be getting into NLN soon.
J. Kissel, O. Patane, B. Lantz After seeing my post of the current (2025-03-19) performance of the H1ISIBS in LHO:83470, Brian -- in his LHO:83473 comment -- rightly cautioned Oli to beware the difference between (1) a "statistical" or "incoherent" model of the CART2EUL projection to the suspension point, where . one takes the ASDs of the CART DOFs (which are inherently only containing amplitude information, no phase relation between channels), . multiplies them by the CART2EUL coefficients, and . takes the quadrature sum to form an ASD model of the euler basis motion, vs. (2) a "linear combination" or "coherent" model of the CART2EUL project to the suspension point, where . the time-series of each CART DOF are multiplied by the CART2EUL coefficients, . the time-series are then coherently summed (where "coherently" summed just means the amplitude AND phase relationship between the channels has been preserved), and . then an ASD is taken of that to form an ASD model of the euler basis motion. He states - "if the DOFs are independent (which maybe they are, and maybe they are not), then using the quadruture sum of the ASDs, (1), is a reasonable thing to do." and - "I think this difference [between (1) and (2)] not going to impact any of your calculations" I'd not seen a comparison of these two models either at all or in a long time, every chamber + SUS combination is different, and I had the data, so I made the comparison. I'll discuss the 6 Euler Basis plots in reverse-traditional order, because they're easiest to understand progressively that way. YAW This plot is uninteresting, because the BS projection matrix from CART to EUL has only one unity element, mapping RZ directly to Yaw. However, it lets me introduce what I'll be plotting. In the upper panel, this shows the both models of ASDs and the underlying Cartesian components multiplied by the CART2EUL matrix element. As expected here, the thick black dashed ASD -- the coherent sum (2) model -- is identical to that think magenta dashed ASD -- the incoherent sum model (2). The lower panel is the ASD ratio of the linear sum (2) divided by the incoherent sum (1). Of course, for this DOF, the two models are identical, so this ASD ratio is identically 1.0 across the whole frequency band. With me so far? Good. :-P PITCH Here, because the Beam Splitter suspension is mounted in the center of the ISI BS optical table, yaw'd 45 degrees, RX and RY map to PITCH via sqrt(2) with the same sign. But the RX and RY performance of the ISI BS is slightly different, so the ratio between (2) and (1) is interesting. Most notably around the HEPI cross-beam foot resonance (traditionally called the "HEPI Pier resonance" prior to 2014; see LHO:13505) -- the broad feature at ~7 Hz -- where the ASD ratio shows that the incoherent sum model (1) under predicts Sus. Point displacement by a factor of ~1.35x w.r.t. the coherent sum model (2). And then at some other feature at ~17 Hz, the incoherent sum model (1) is over predicting the Sus. Point displacement by ~(1/0.8) = 1.25x. ROLL OK, now flip the sign of the contribution of RY, and watch the coherent sum drop -- fascinating! The contribution of that same ~7 Hz feature is now dramatically over-predicted by the incoherent sum, by a factor of ~(1/0.4) = 2.5x. Are these two the inverse of each other? No! I don't show it explicitly, but comparing (2)/(1) for roll (the inverse of what's plotted) and (1)/(2) for pitch, the 7 Hz number is 0.74x and 0.52x respectively, so markedly different! VERTICAL Now we're getting really interesting -- for vertical, Z is mapped one-to-one, but RX and RY are contributing in opposite sign, and with only *roughly* the same magnitude [m/rad] CART2EUL coefficient. The incoherent sum (1) is overestimating the vertical displacement by as much as a factor of ~(1/0.2) = 5x where the vertical motion is limited by RX and RY between 0.5 and 3 Hz. Wow! I won't look type thru the rest of the plot, because the plot describes it best, but boy is it more interesting than I thought it would be. TRANSVERSE With transverse, even though this degree of freedom "doesn't matter" for the beam splitter, now we're cooking with 5 contributing Cartesian degrees of freedom and except for RZ they're all contributing at interesting levels. Again, you reading the plot is more useful than me describing it here, but it's quite interesting that the linear sum (2) predicts more motion between 0.6 Hz and 3.5 Hz and the incoherent sum (1) predicts more motion overestimates the motion between 3.5 to 15 Hz. LONGITUDINAL Finally, the DOF we work the hardest on, shows contribution from all 5 Cartesian degrees of freedom. A lucky-coincidence perhaps, but it looks like the models are about the same for most of the frequency region, and the incoherent sum (1) is over-predicting the displacement between 3.5 to 15 Hz, which is re-enforcing Brian's comment. WHAT DOES IT ALL MEAN? Brian is, again, definitely right to call out that the linear sum (1) model is a better model of the displacement of the Sus. Point than the incoherent sum. But, both I (and perhaps even he) definitely wasn't expecting factors of 2x discrepancy, let alone factors of 5x. So, I think I might make Brian's conclusion from LHO:83473 a little stronger -- the difference between models will impact the calculations of the Bigger Beam Splitter Suspension (BBSS) performance, so for the update to the seismic input motion, I'll *not* just update the performance from the ~2005 seisBSC.m estimate to the current 2025 real *cartesian* performance incoherently projected to the Sus Point, but instead update it to the current 2025 real *euler* Sus. Point performance computed in the front-end.
Brian says: "huh. I'm not happy about being right here. Something is wrong with that ISI. This means there is very strong coupling between Z and RX/RY on that table, something I've been worried about for a while, but not able to improve. This was just supposed to be a 'thing to keep in mind when checking your work'." This forced me to look at my own plots again with a different lens, that I think is worth sharing: "Mmm -- maybe you're thinking too fast here -- the RX/RY coupling to Sus Point Vertical is entirely via geometry, not anything funky with the cross-coupling within the ISI DOFs. Sure, improving RX/RY would help by whatever way you want, but this doesn't point fingers at any internal, ISI, RX/RY to Z (or vice verse) coupling. But also -- the good news is that we "improve" the Sus. Point vertical motion for the BS by a factor of 5x at 0.5 Hz just by showing the better math'ed projection! And actually -- now that I stare at the V plot more closely, the *coherent* V motion (the black-dashed trace) is not limited by RX or RY *anywhere*: - Where the RY/RX component motion is comparable to Z component (say, between 0.5 Hz and 3 Hz), apparently, the *differential* RX / RY motion is smaller than the component, and - Where the RX/RY component motion is clearly different from each other (between 5 and 30 Hz), the Z motion is far larger anyways." But, back to Brian's worry about this ISI's performance -- remember to head to LHO:83530 for discussion :: yes, this is one of the worst performing ISIs and we don't know why.
The Kepco Power Supply for SUS-C4 started chirping at the end of maintenance today. By 2pm the chirping is more regular. The draw on the supply is 7A, typical failing fans last a few days once they get to this stage. We should replace this one before the weekend, as a target of opportunity. Down time will be 30 mins start to finish.
M. Pirello, F. Clara
Due to earthquake we took a window of opportunity to replace the SUS-C4 Kepco Power Supply which controls HAM1 and HAM2 suspensions. These suspensions were placed into safe and the supply replaced. We replaced only the -18V supply, the +18V matching supply was replaced in December 2022 so we left it in place.
M. Pirello, F. Clara
FranciscoL, TonyS, MattT, RickS
On Tuesday, March 25, we reverted the PCALX lower beam to its nominal center. We expect to see a change of 4 HOPs in \chi_XY -- returning to the value it was two week ago.
Target was placed with a 33 degree offset as seen on the first attachment (TARGET_ON -- featuring a responsible scientist, wearing laser goggles). Each individual beam voltage values, as found, were very similar to the values recorded at the end of the move done last week.
The following table shows the voltage values as read by the Keithley voltmeter we use during the procedure
Step | Comment | Readout [V] |
---|---|---|
1 | Both beams - target off | 3.379 |
2 | Both beams - target on (as found) (BEFORE_MOVE) | 2.937 |
3 | Lower beam after actuation | 1.395 |
4 | Both beams - target on (AFTER_MOVE) | 2.903 |
5 | Both beams - target off | 3.394 |
The IFO has not regain lock at the time of writing this alog which limits further observations from this move.
WP 12393
The FE and IO chassis for h1seih16 were powered down for in-rack cabling of the ISI electronics. All cables are now routed and dressed. The long field cables were left disconnected, will wait until they are in connected at the flange.
The AI chassis on U38 was removed. AA chassis from U39 was moved down. This matches LLO's rack configuration, alog 75328.
CDS Team
RyanC, TJ
I wrote a new decorator in ISC_library (@ISC_library.bring_unlocked_imc_2w_decorator(nodes)) for the specific scenario of the IMC losing lock while we're at 10Ws which would give it trouble relocking - alog82436. The decorator looks for the IMC being unlocked with a power above 2Ws and if the rotation stage is stationary it requests the LASER_PWR GRD to 2Ws.
We sprinkled the decorator into ALIGN_IFO, INIT_ALIGN, into the MICH, SRC and AS_CENTERING states, I also added it to CHECK_MICH_FRINGES and MICH_OFFLOADED in ISC_LOCK. We successfully tested it today during an initial alignment by breaking the IMC lock during these states.
Tue Mar 25 10:12:47 2025 INFO: Fill completed in 12min 43secs
TITLE: 03/25 Day Shift: 1430-2330 UTC (0730-1630 PST), all times posted in UTC
STATE of H1: Lock Acquisition
OUTGOING OPERATOR: Ibrahim
CURRENT ENVIRONMENT:
SEI_ENV state: CALM
Wind: 5mph Gusts, 3mph 3min avg
Primary useism: 0.03 μm/s
Secondary useism: 0.25 μm/s
QUICK SUMMARY: H1 is currently relocking up to MOVE_SPOTS. Looks like H1 was able to lock twice last night and most recently lost lock about an hour ago. Maintenance day today, but I'll let H1 continue until those activities begin.
Halted locking for the start of maintenance day. ISC_LOCK to 'IDLE' and seismic environment to 'MAINTENANCE' at 14:40 UTC.
Power cycling the dust monitor did not help, later in the day I restarted the IOC using telnet which was successful.
Workstations were updated and rebooted. Os packages were updated, and conda packages were also updated.
In the CDS conda environment, gwpy was upgraded to version 3.0.12. Among other improvements, this version fixes an issue that could cause matplotlib to lock up while creating pltos after importing gwpy.
IFO is in LOCKING at FIND_IR
I got called at 03:11 AM because ALSY Guardian went into fault during initial alignment and stayed there for an hour at which point IFO Notify was triggered to call the OWL Ops. I couldn't see anything immediately wrong with Y-ARM other than it got itself into a weird state. Long story short, the ALSY IR DC Power is low, and around the threshold for ALSY guardian faulting.
I went into init to try another initial alignment but ALSY got into the same state. Upon further investigaiton, this was due to the ALS Guardian detecting an error in the locking relating to the ALS_Y_LASER_IR_DC. I noticed that ALSY would only fault if the power went below 4.5 mW, which I later realized to be on the boarder, fluctuating between "too low" and over 4.5. I set the threshold on the same page (attached pic) to 4.48 (lower by 0.02mW), which seems to have fixed the issue. I waited until ALS Locked in both INITIAL_ALIGNMENT and LOCKING_ARMS_GREEN to ensure that the fix worked. I waited a bit more and can confirm we can lock DRMI (we lost lock a few minutes thereafter though).
I have accepted and screenshoted the SDF corresponding to the power change in SAFE.SNAP just in case we lose lock on the way to NLN (since this gets reset with each LL). I will likely get called again and need to accept the SDF in OBSERVE later, though that may be during DAY OPS time. Other screenshots have been attached, including the screen where I made the power threshold change. I've re-set my OWL and will stay logged in to expect a call for potential SDF confirmation.
Accepted ALSY IR DC Power Change in OBSERVE (attached). H1 is now OBSERVING.
Ryan Short, Sheila
Last November the power out of this laser dropped 13% after the current was reduced to get it operating in a more stable region during the PSL NPRO difficulties, 81117. Daniel lowered some thresholds and raised some gains at the time, but not the ALS Y LASER IR threshold. It has been close to the limit since but only drifted below last night, due to it's normal long slow drift. I've lowered the threshold to 4 mW now, so that we have a similar level of headroom for this error as we did before the laser current drop. I've accepted this in safe.snap but not in observe
Ryan Short also has been looking at some of our other ALS locking problems. He noticed that sometimes the ALS PLL beckhoff gives an error based on the reference cavity transmission. This is leftover from when the ALS pick off was in transmission of the reference cavity, but it has been moved so this error check isn't helpful anymore. We've set the threshold to -1 for ALS X and Y H1:ALS-Y_FIBR_LOCK_REFCAV_TRANSLIM, and also accepted these in safe.snap, but not observe.
TITLE: 03/24 Eve Shift: 2330-0500 UTC (1630-2200 PST), all times posted in UTC
STATE of H1: Lock Acquisition
INCOMING OPERATOR: Ibrahim
SHIFT SUMMARY:
Rough shift with DRMI locking all of a sudden being VERY finicky. Hoping POPAIR gain change helps with locking (after the end-of-shift-alignment).
LOG:
The shift started with Ryan looking into why ALSy was causing grief in the afternoon (it would later clear up on its own), but since the beginning of the EVE shift, DRMI locking has been the issue.
Have went through 2-Initial Alignments, as well as several successful PRMIs and CHECK MICH FRINGES.
DRMI Symptoms:
DRMI would start out the first few seconds with strong flashes seen on the camera and decent flashes on ndscopes, but
Then the behavior would switch to an ugly camera image which would be seen as DRMI looking like it's going to catch, but within 1-sec POP18+90 (and also the camera) would "wobble" back down to zero in a "slow flash".
(It feels like DRMI has been like this over the weekend as well, but after some of these wobbles to zero after these "slow flashes," DRMI would lock. Not the case tonight---have had zero DRMI locks going on 6+hrs.)
It feels like the alignment is decent, and no environmental issues, but it doesn't seem to trigger or start LSC control when these flashes start (hence their "slow" drop of POP18+90.).
What's Been Tried:
Now: We Wait
Just before Sheila and I were going to go with this new gain, a M6.7 EQ rolled through (of course). Probably have another 30-90 min before the ground calms down, but the hope is we'll have the same luck Elenna, Ibrahim, and Sheila had on March 4th with DRMI locking right up!
I'm looking again at the OSEM estimator we want to try on PR3 - see https://dcc.ligo.org/LIGO-G2402303 for description of that idea.
We want to make a yaw estimator, because that should be the easiest one for which we have a hope of seeing some difference (vertical is probably easier, but you can't measure it). One thing which makes this hard is that the cross coupling from L drive to Y readout is large.
But - a quick comparison (first figure) shows that the L to Y coupling (yellow) does not match the Y to L coupling (purple). If this were a drive from the OSEMs, then this should match. This is actuatually a drive from the ISI, so it is not actually reciprocal - but the ideas are still relevant. For an OSEM drive - we know that mechanical systems are reciprocal, so, to the extent that yellow doesn't match purple, this coupling can not be in the mechanics.
Never-the-less, the similarity of the Length to Length and the Length to Yaw indicates that there is likely a great deal of cross-coupling in the OSEM sensors. We see that the Y response shows a bunch of the L resonances (L to L is the red TF); you drive L, and you see L in the Y signal. This smells of a coupling where the Y sensors see L motion. This is quite plausible if the two L OSEMs on the top mass are not calibrated correctly - because they are very close together, even a small scale-factor error will result in pretty big Y response to L motion.
Next - I did a quick fit (figure 2). I took the Y<-L TF (yellow, measured back in LHO alog 80863) and fit the L<-L TF to it (red), and then subtracted the L<-L component. The fit coefficient which gives the smallest response at the 1.59 Hz peak is about -0.85 rad/meter.
In figure 3, you can see the result in green, which is generally much better. The big peak at 1.59 Hz is much smaller, and the peak at 0.64 is reduced. There is more from the peak at 0.75 (this is related to pitch. Why should the Yaw osems see Pitch motion? maybe transverse motion of the little flags? I don't know, and it's going to be a headache).
The improved Y<-L (green) and the original L<-Y (purple) still don't match, even though they are much closer than the original yellow/purple pair. Hence there is more which could be gained by someone with more cleverness and time than I have right now.
figure 4 - I've plotted just the Y<-Y and Y<-L improved.
Note - The units are wrong - the drive units are all meters or radians not forces and torques, and we know, because of the d-offset in the mounting of the top wires from the suspoint to the top mass, that a L drive of the ISI has first order L and P forces and torques on the top mass. I still need to calculate how much pitch motion we expect to see in the yaw reponse for the mode at 0.75 Hz.
In the meantime - this argues that the yaw motion of PR3 could be reduced quite a bit with a simple update to the SUS large triple model, I suggest a matrix similar to the CPS align in the ISI. I happen to have the PR3 model open right now because I'm trying to add the OSEM estimator parts to it. Look for an ECR in a day or two...
This is run from the code {SUS_SVN}/HLTS/Common/MatlabTools/plotHLTS_ISI_dtttfs_M1_remove_xcouple'
-Brian
ah HA! There is already a SENSALIGN matrix in the model for the M1 OSEMs - this is a great place to implement corrections calculated in the Euler basis. No model changes are needed, thanks Jeff!
If this is a gain error in 1 of the L osems, how big is it? - about 15%.
Move the top mass, let osem #1 measure a distance m1, and osem #2 measure m2.
Give osem #2 a gain error, so it's response is really (1+e) of the true distance.
Translate the top mass by d1 with no rotation, and the two signals will be m1= d1 and m2=d1*(1+e)
L is (m1 + m2)/2 = d1/2 + d1*(1+e)/2 = d1*(1+e/2)
The angle will be (m1 - m2)/s where s is the separation between the osems.
I think that s=0.16 meters for top mass of HLTS (from make_sus_hlts_projections.m in the SUS SVN)
Angle measured is (d1 - d1(1+e))/s = -d1 * e /s
The angle/length for a length drive is
-(d1 * e /s)/ ( d1*(1+e/2)) = 1/s * (-e/(1+e/2)) = -0.85 in this measurement
if e is small, then e is approx = 0.85 * s = 0.85 rad/m * 0.16 m = 0.14
so a 14% gain difference between the rt and lf osems will give you about a 0.85 rad/ meter cross coupling. (actually closer to 15% -
0.15/ (1 + 0.075) = 0.1395, but the approx is pretty good.
15% seem like a lot to me, but that's what I'm seeing.
I'm adding another plot from the set to show vertical-roll coupling.
fig 1 - Here, you see that the vertical to roll cross-couping is large. This is consistent with a miscalibrated vertical sensor causing common-mode vertical motion to appear as roll. Spoiler-alert - Edgard just predicted this to be true, and he thinks that sensor T1 is off by about 15%. He also thinks the right sensor is 15% smaller than the left.
-update-
fig 2- I've also added the Vertical-Pitch plot. Here again we see significant response of the vertical motion in the Pitch DOF. We can compare this with what Edgard finds. This will be a smaller difference becasue the the pitch sensors (T2 and T3, I think) are very close together (9 cm total separation, see below).
Here are the spacings as documented i the SUS_SVN/HLTS/Common/MatlabTools/make_sushlts_projections.m
I was looking at the M1 ---> M1 transfer functions last week to see if I could do some OSEM gain calibration.
The details of the proposed sensor rejiggling is a bit involved, but the basic idea is that the part of the M1-to-M1 transfer function coming from the mechanical plant should be reciprocal (up to the impedances of the ISI). I tried to symmetrize the measured plant by changing the gains of the OSEMs, then later by including the possibility that the OSEMs might be seeing off-axis motion.
Three figures and three findings below:
0) Finding 1: The reciprocity only allows us to find the relative calibrations of the OSEMs, so all of the results below are scaled to the units where the scale of the T1 OSEM is 1. If we want absolute calibrations, we will have to use an independent measurement, like the ISI-->M1 transfer functions. This will be important when we analyze the results below.
1) Figure 1: shows the full 6x6 M1-->M1 transfer function matrix between all of the DOFs in the Euler basis of PR3. The rows represent the output DOF and the columns represent thr input DOF. The dashed lines represent the transpose of the transfer function in question for easier comparison. The transfer matrix is not reciprocal.
2) Finding 2: The diagonal correction (relative to T1) is given by:
I will post more analysis in the Euler basis later.
Here's a view of the Plant model for the HLTS - damping off, motion of M1. These are for reference as we look at which cross-coupling should exist. (spoiler - not many)
First plot is the TF from the ISI to the M1 osems.
L is coupled to P, T & R are coupled, but that's all the coupling we have in the HLTS model for ISI -> M1.
Second plot is the TF from the M1 drives to the M1 osems.
L & P are coupled, T & R are coupled, but that's all the coupling we have in the HLTS model for M1 -> M1.
These plots are Magnitude only, and I've fixed the axes.
For the OSEM to OSEM TFs, the level of the TFs in the blank panels is very small - likely numerical issues. The peaks are at the 1e-12 to 1e-14 level.
@Brian, Edgard -- I wonder if some of this ~10-20% mismatch in OSEM calibration is that we approximate the D0901284-v4 sat amp whitening stage with a compensating filter of z:p = (10:0.4) Hz? (I got on this idea thru modeling the *improvement* to the whitening stage that is already in play at LLO and will be incoming into LHO this summer; E2400330) If you math out the frequency response from the circuit diagram and component values, the response is defined by % Vo R180 % ---- = (-1) * -------------------------------- % Vi Z_{in}^{upper} || Z_{in}^{lower} % % R181 (1 + s * (R180 + R182) * C_total) % = (-1) * ---- * -------------------------------- % R182 (1 + s * (R180) * C_total) So for the D0901284-v4 values of R180 = 750; R182 = 20e3; C150 = 10e-6; C151 = 10e-6; R181 = 20e3; that creates a frequency response of f.zero = 1/(2*pi*(R180+R182)*C_total) = 0.3835 [Hz]; f.pole = 1/(2*pi*R180*C_total) = 10.6103 [Hz]; I attach a plot that shows the ratio of the this "circuit component value ideal" response to approximate response, and the response ratio hits 7.5% by 10 Hz and ~11% by 100 Hz. This is, of course for one OSEM channel's signal chain. I haven't modeled how this systematic error in compensation would stack up with linear combinations of slight variants of this response given component value precision/accuracy, but ... ... I also am quite confident that no one really wants to go through an measure and fit the zero and pole of every OSEM channel's sat amp frequency response, so maybe you're doing the right thing by "just" measuring it with this technique and compensating for it in the SENSALIGN matrix. Or at least measure one sat amp box's worth, and see how consistent the four channels are and whether they're closer to 0.4:10 Hz or 0.3835:10.6103 Hz. Anyways -- I thought it might be useful to be aware of the many steps along the way that we've been lazy about the details in calibrating the OSEMs, and this would be one way to "fix it in hardware."
The new clean air supply (compressor, tank, dryer and a series of extra filters), which was received in the end of 2024, was installed in the EX mechanical room as a replacement for the old system. The installation work was carried out in the last few weeks, the last step - the startup by Rogers Machinery - happened today. This new system has a 69 cfm air delivery operating with 3 pcs. of 7.5 HP motors (in sum 22.5 HP). In comparison, the old system had a 50 cfm air delivery, operating with 5 pcs. of 5 HP motors (in sum 25 HP). Moreover, the new system (unlike the old one) has an automatic dew point monitor, and a complete pair of redundant dryer towers. So, this new system is a major improvement. The reason for this 69 cfm limit (and not more) is that the cooling of the compressor units in the MER is still feasible, moreover, the filters and the airline do not need any upgrades, they can still accommodate the airflow. Both the new and old systems are able to produce at least -40 deg F dew point air on paper. During the startup, the new system was however able to produce much better than this - it was ~-70 deg F (and dropping) - as you can see in the attached photo. Last but not least, a huge congratulations to the Vacuum team for the installation, as this was the first instance, when the installation of a clean air system was carried out by LIGO staff, so this is indeed a huge achievement. Also, big thanks to Chris, who cleaned some parts for the compressor, to Tyler, who helped a lot in the heavy lifting, and to Richard & Ken, who did the electrical wiring. From next week on, we repeat this same installation at the EY station.