J. Oberling, R. Savage, E. Merilh
Noting some of the recent issues with RefCav relocking, we went into the PSL to take some measurements of the FSS to see if we could gather some clues as to what's going on. We began by taking a transfer function and immediately noticed something odd, see first attachment (FSS2.tif). Out around 775kHz there is a large bump that rises above the UFG (please recall that the UGF for the FSS is read at -10dB due to the design of the TTFSS electronics; in this case it is just below 500kHz), with a corresponding bump in the phase. Looking at the last TF we took, the bump in magnitude was present, but smaller than it is now, with no corresponding bump in the phase; this therefore, is a change in the TF since mid-December. Zooming in on the area (2nd attachment, FSS3.tif) shows it to be more than a simple bump, but a series of them culminating in a large hump at ~776kHz that rises almost 10dB above the UGF. We took a spectrum of the IN1 port on the TTFSS (closest to the mixer) and while it looked a bit "spikey" (for lack of a better word), the area around the hump looked different; more flat, but with a dip and return (with a spike in the middle of this), followed by a small bump (see third attachment, FSS6.tif). Thinking this could be an indication of an issue with the NPRO noise eater (the noise eater (NE) supresses the natural relaxation oscillation of the NPRO crystal, which tends to hang out in this area (each laser is different)), so we repeated the IN1 spectrum with the noise eater ON and OFF; see 4th and 5th attachments, FSS8.tif (NE OFF) & FSS9.tif (NE ON). As can be seen, the relaxation oscillation peaks around 928kHz, with the hump starting above 800kHz and ending around 1MHz; with the NE ON, the relaxation oscillation disappears; in both, the area below 800kHz is unchanged,indicating that the NPRO NE is not the problem.
We're still digesting this info, but having a hump beyond the UGF that pops up above it is likely the underlying cause of our recent FSS instabilities; at this point we're not sure what's causing this. Rick suspects that we may have some kind of parallel path resonance happening, or maybe there's a notch in this version of the TTFSS that we need to re-tune. I've added 1 final picture, FSS13.tif. In this pic the marker is at the current FSS UGF of ~486kHz; at 10dB/div, it is very clear that this feature at 776kHz is at least 10dB above the UGF. Investigation continues.
TITLE: 01/30 Eve Shift: 00:00-08:00 UTC (16:00-00:00 PST), all times posted in UTC
STATE of H1: Observing at 115Mpc
OUTGOING OPERATOR: Jim
CURRENT ENVIRONMENT:
SEI_CONF state: WINDY
Wind: 10mph Gusts, 7mph 5min avg
Primary useism: 0.09 μm/s
Secondary useism: 0.50 μm/s
QUICK SUMMARY: We have been in observing fro 30 minutes.
TITLE: 01/30 Day Shift: 16:00-00:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Observing at 119Mpc
INCOMING OPERATOR: Camilla
SHIFT SUMMARY:
LOG:
16:15 Lockloss
18:00 Kyle Gerardo to EY
20:49 Sheila starting squeezer commissioning
21:20 Back to observing
22:10 More squeezing work
23:40 Back to Observe
After having trouble earlier (54819), we were able to scan the squeezer with 13.7mW of injected green power. I will make plots with the correlated noise subtracted and post them when ready.
Earlier in this lock our range was ~116Mpc, but we saw during the scan that for CLF demod angles aroun 105degrees we could get 120 Mpc. We have left the injected power at 13.7mW and the demod angle at 105 to get a few extra Mpc.
Sheila had to back out of some work on the squeezer. She wasn't able to get the squeezer back up, so we not squeezing right now. This has dropped our range down to ~100 mpc. Not sure when the commissioners will be able to recover.
Gerardo M., Kyle R.
This was a T.O.O. task as the IFO was out-of-lock.
This new Turbo is slated to be installed during this upcomming (8 hour) maintenance Tuesday. Having moved this to the EX prior to Tuesday will greatly improve the likelyhood that we can complete the installation within the alotted 8hrs.
Back in October, I had worked on the BS St2 boosts to try to reduce locklosses caused by engaging the ST2 loops. I had noticed a few times that we still got kicks here, and I had a lockloss earlier today. I reduced the ramp times on the boosts for the X Y Z and RZ loops to 2 seconds, from 3. The last couple of DRMI acquisitions have had this change running, and I haven't noticed the wiggles in DRMI that I was seeing before. I'll try to get a more detailed look, after we get locked again.
While H1 is out of lock I restarted the lv_alert external alert service on the ext-alert virtual machine. This is the second time I have had to do this this week.
This looks to be the known issue of the LVAlert subscriptions silently disappearing (I can't seem to find the link to where the bug is reported). This used to happen once in a blue moon, but lately it seems to be more frequent.
I talked with Jonathan and I'll write a script to monitor the heartbeat and then restart the systemd process if it flatlines. This should automatically take care of the resubscribing to the LVAlert nodes that we need.
In the mean time, Operators if you see the "GraceDb Query Failure" icon on the ops overview, please see the wiki in the follow link for instructions to restart the LVAlert service. https://cdswiki.ligo-wa.caltech.edu/wiki/RestartingLVAlert
TITLE: 01/30 Owl Shift: 08:00-16:00 UTC (00:00-08:00 PST), all times posted in UTC
STATE of H1: Earthquake
INCOMING OPERATOR: Jim
SHIFT SUMMARY:
H1's been locked 7+hrs with decent range. SEI_CONF is in WINDY.
GraceDB query failure continues. I asked LLO (talked to Doug L & later Danny S----thanks to both of you!!) to give us any notifications they receive. I sent an email about this to LHO CDS Admin.
LOG:
Received an FMCS Air Handler Alarm, but trends (attached) of the air handler and chiller at MY look reasonable.
Fairly smooth running of H1 with 3+hrs of lock. There is an inbound Mediterranean 5.9 EQ, so will be monitoring. GraceDB is still down here at LHO.
After the lockloss at ENGAGE SOFT LOOPS, I made sure to have ndscopes for ASC & ADS Lines up to watch for the next lock.
Sure enough, made it through with no issues at Soft Loops. Next scary spot lately has been LOWNOISE_ASC, but we made it through there with no issues.
Not sure what helped with getting to NLN, but will note the following:
P.S. Had teeny tiny 10^-17 SDF diffs for a couple of ALS channels, so I ACCEPTED (diffs are attached).
I have modified the scripts that write these values to ensure that they get rounded also in the case of a ctrl-c exit, so hopefully we won't see these anymore. When I check the Xarm green initial alignment setpoints on Tuesday, I will test the new rounding.
TITLE: 01/30 Owl Shift: 08:00-16:00 UTC (00:00-08:00 PST), all times posted in UTC
STATE of H1: Earthquake
OUTGOING OPERATOR: Camilla
CURRENT ENVIRONMENT:
SEI_CONF state: USEISM
Wind: 5mph Gusts, 3mph 5min avg
Primary useism: 0.05 μm/s
Secondary useism: 0.69 μm/s
Microseism looks like it's started a decrease over the last 4hrs.
QUICK SUMMARY:
TITLE: 01/30 Eve Shift: 00:00-08:00 UTC (16:00-00:00 PST), all times posted in UTC
STATE of H1: Earthquake
INCOMING OPERATOR: Corey
SHIFT SUMMARY: Lockloss (maybe) from a 5.1M EQ in Mexico. Passing off to Corey with DRMI locked.
LOG:
[Camilla, Jenne, Sheila, Keita]
Camilla had several locklosses at ENGAGE_SOFT_LOOPS again tonight. Normally the remedy is to go back and do another initial alignment, but Sheila pointed out that in all of the lock attempts the Yarm isn't arriving at the engage ASC states very close to the correct alignment. Since this has been true even after fresh initial alignments, this is indicative of the inital alignment setpoints not being very good.
We checked, and this is not at all related to the camera network/freezing issues of late. Every time the camera setpoints come back correctly to the values that were last changed at the end of October. So, this is likely just that things have drifted over the last ~3 months and the initial alignment setpoints just needed updating.
Since we had been failing to even engage the soft loops, we hand-moved the Yarm soft using the script ....userapps/asc/h1/move_ARM_dev.py in steps of "YS P 0.03" to get the ADS DOF 5 Pit a bit closer to zero. When it was off the limiter rail (but not yet all the way to zero), we let the guardian finish the soft loop alignment to the centers of the optics by letting it do ENGAGE_SOFT_LOOPS. Once all of the soft loops had converged, we checked that the Yarm green was resonating the TEM00 mode, and saw that the green WFS and camera values were not close to zero. So, we ran the script ....userapps/als/h1/scripts/setEndGreenQPDOffsets_YARM.py to change the WFS centering setpoints, and once that was finished we also set the camera values.
The Xarm green didn't want to catch the 00 mode, and since the Xarm ADS hasn't been a problem we elected to go forward with locking. We lost lock later in the sequence, so did an initial alignment to confirm that we can reacquire with these updated Yarm initial alignment setpoints. I have on the board to check the Xarm setpoints on Tuesday after maintenance.
Attached are screenshots of the new values, and the old values.
Alog 50968 has a sketch of the procedure on how to update initial alignment references.
I've added rounding to the move_ARM_dev script, and I have added a try-except clause to the setEnd offsets scripts, so hopefully we won't see as many rounding SDF diffs in the future. I'll test these on Tues.
We were out of observing for ~40 minutes this afternoon while Daniel and I measured the spectrum of the DCPDs up to 4MHz. The goal of this was to see if it is plausible that noise from the interferometer (laser) around 3MHz is beating with the coherent locking field (at 3.125 MHz) and downconverting to create the noise we see when we have a more power in the coherent locking field. Indeed, there is a lot of noise at high frequencies. Calibrated plots coming soon.
Here is a plot of the data taken from the DCPDs up to 4MHz. I've removed the 20dB of gain and the poles at 265kHz and 290kHz from D1700376 in this plot. This was measured with our usual darm offset, restuling in 10mA on each of the DCPDs (we used one of the single PD outputs from D1700376). We tried to repeat this measurement with a diode set up in the AS air path yesterday, 54636, but the 3.125MHz peak was only 20dB above the noise level, so we weren't able to see any of the other noise apparent in this measurement.
Thanks, this is useful for ongoing CLF work.
For reference, Koji's measurements of the transimpedance are below. You can see that the rolloff flattens a bit in the MHz, so I'm less certain how real the bump is.
https://nodus.ligo.caltech.edu:8081/OMC_Lab/236
https://nodus.ligo.caltech.edu:8081/OMC_Lab/235
does your RF equipment have the ability to make a decently long cross correlation? That is surely what we need if we can conveniently get equipment to do it. Alternatively, you may be able to take spectra simultaneously in a sum and null output configuration, and then subtract them. It won't be as clean as xcorr, but it will show excess in a way that is less succeptible to systematic errors from inverting the PD response. Sum can be picked off from the SQZ chassis, and null just needs the phase shift before an RF splitter used in reverse (depending on the phase convention of the splitter).
Update, I remembered that I had acquired the LISO model and fit it in IIRrational for just these kinds of occasions. These fits should be decent up to 10MHz where the simulation cut off.
scipy ZPK notation:
(array([-1.09367517e+06+9.16935186e+04j, -1.09367517e+06-9.16935186e+04j,
-4.54321270e+01+3.94631525e-01j, -4.54321270e+01-3.94631525e-01j,
-2.85835003e+07+0.00000000e+00j]), array([-1.12584306e+07+1.59926553e+07j, -1.12584306e+07-1.59926553e+07j,
-3.11667017e+07+1.49827313e+08j, -3.11667017e+07-1.49827313e+08j,
-4.41594538e+07+5.59042545e+07j, -4.41594538e+07-5.59042545e+07j,
-1.51046460e+07+2.52263715e+07j, -1.51046460e+07-2.52263715e+07j,
-1.02822684e+05+0.00000000e+00j, -9.54273138e+04+0.00000000e+00j,
-5.08417603e+02+0.00000000e+00j, -4.91824766e+02+0.00000000e+00j]), 2.71124765615596e+56)
foton notation:
ZPK([
-174063.80969071676 + 14593.476738924443*i; -174063.80969071676 - 14593.476738924443*i;
-7.2307475830315395 + 0.06280755795247621*i; -7.2307475830315395 - 0.06280755795247621*i;
-4549205.365087142;
],[
-1791834.8749338891 + 2545310.1382306265*i; -1791834.8749338891 - 2545310.1382306265*i;
-4960334.630691198 + 23845757.522465646*i; -4960334.630691198 - 23845757.522465646*i;
-7028195.359231514 + 8897438.443450466*i; -7028195.359231514 - 8897438.443450466*i;
-2403979.0673290133 + 4014901.7200727463*i; -2403979.0673290133 - 4014901.7200727463*i;
-16364.738450407038; -15187.728699344743;
-80.91717459920993; -78.27634271397135;
], 2.71124765615596e+56, "f")
Attached are the fits and the output of the LISO model. I think the model differs a touch from Koji's measurements on the exact 3MHz cutoff frequency.
Here is a plot (and the data used to make it) of the DCPD output measured with the analyzer in noise mode. The first set of data (in the original log above) were taken in spectrum mode. The dark noise in this new plot was measured durring Friday's EQ in Turkey, the "squeezer blocked" trace was taken durring the commisioning time Thursday (54681). These are calibrated using the filters in D1700376 and Lee's estimate of the OMC DCPD transimpedance above. Both spectra were taken with 30Hz resolution bandwidth and 3Hz video bandwidth. A potential problem with this measurement could be that the squeezer came unlocked and the beam diverter closed partway through the measurement, although that didn't seem to have an impact on the spectrum here.
It does seem suspicous that the quadrature difference, which should represent noise coming from the interferometer light, has a spectrum so similar to the dark noise.
This appears qualitatively a bit different than the post-demodulation measurement of the spectrum at LLO50307. There the blocked and dark noise ASD's changed by a factor of about 1.5. This appears to be substantially less than that at 3.125MHz.
Here is one more plot of the DCPD spectrum up to high frequency, again. In the original version of the attached plot in 54753 I made two mistakes in the calibration, which are fixed here..
The attached plot shows, in addition to the dark noise and locked spectrum, the level of amplitude noise which I think would be needed to create downconverted noise about equal to the current shot noise limited sensitivity. One conclusion is that the dark noise of the DCPDs at 3MHz is too high for us to measure the level of amplitude noise that we need to measure to be sure that we can turn up the CLF power to the level required for the filter cavity controls. However, the difference between the in lock and the dark noise spectrum suggests that the current level of amplitude noise is well above this level, such that it should be dominating the noise in DARM. So something seems to be wrong either with the measurement or with my projections.
One could worry that there might be significant variation between the individual transimpednce amplifiers at 3MHz. We have a measurement made at 3.12MHz with the installed amplifier: 47540 which is roughly consistent with the one that Koji measured and Lee's fit above. Another worry could be that we are running with a different transimpedance than these measurements were taken with, but we are running in high Z which is 400 Ohms at DC according to D060572, My plot of Lee's fit above gives a DC transimpedance of 200 Ohms, but it is ~220 Ohms at 3.125 MHz, so I think it is close enough.
While RGA manufacturer was on site testing Labview-based RGA software, we noticed a significant AMU 28 peak at EX, towering water signature, suggesting an air leak. The total pressure is 1.9e-9 Torr and the trend is relatively flat, so no urgent concern. I suspect this is due to the failed annulus ion pump on GV20. We may have an inner o-ring leak on GV20 in addition to diffusion through o-rings.
AIP has been off for over a week as EX has been inaccessable due to tumbleweed blockages.
EY scan is also attached for comparison.