Related: alog 22199
We measured the output of the Low Voltage ESD monitor (D1500129) at the AA side at the remote rack using SR785 right after the IFO was locked up again after the maintenance.
No surpise was found, see attached. 'UR', 'UL' etc. are the analog measurements of the corresponding ESD monitor. Noise floor was measured with the inputs of SR785 short circuited.
Don't worry about LR trace, it looks as if it's noisier than the others but it's not, it's just the spectral leakage artefact (somehow I did not save the small BW measurement for LR).
'digital LL signal projected' is H1:SUS-ETMY_L3_MASTER_OUT_LL, but with a correction of 20/2^17 Volt/count for DAC conversion, zpk([50;50;3250], [2.2;2.2;152]) for SUS awhite type filters, and 2 *4.99/(1.2+15+4.99)*zpk([],[40]) for the monitor circuit.
The measurements agree well with the projection up to 1kHz. Higher than that, the SR785 noise dominates, but this should be good enough for our purpose.
What was done:
We disconnected the LV ESD monitor cable (SUS ESD 06) from the front panel of the AA, and connected DB9 breakout board to the cable but not to the AA.
For each quadrant (pin1-6 for UR, 2-7 for LR, 3-8 for UL and 4-9 for LL), we used two clip-BNC cables to connect the positive pin (1, 2, 3 or 4) to A connector of SR785 and negative to B, and the BNC shell was connected to the shell of the DB9 connector on the AA chassis.
SR785 was in A-B mode, AC coupled. The plot doesn't account for the AC coupling, but its roll off is at 0.16Hz and does not affect the plot. Sensitivity was fixed at -8dBVpk.
Low frequency measurements (0-400Hz, 800 lines) were performed for all quadrants but it was not saved for LR. As a result, in the plot it looks as if LR is noisier than the other channels, but in reality it's showing the spectral leakage artefact due to larger bandwidth measurement for f<400Hz.
Higher frequency measurements (0-1.2k and 0-12.8k, 800 lines) were performed and saved for all quadrants.
Only for LL we measured up to 102kHz to make sure that there's no high frequency bump or anything, but all measurements are dominated by SR785 noise for f>1kHz anyway.
Attached is the matlab file containing the voltage data for all quadrants and the SR785 noise.
Um, count-to-voltage DC gain conversion of the DAC is 20Vpp differential per 2^18 counts. So the grandparent entry is incorrect by a factor of 2 there. But I'm measuring the voltage in the differential output stage of LV driver which has the DC gain of 2 (i.e. 10V pp single ended is converted to 10V pp differential), which I didn't account for in the script.
So in the end the conclusion doesn't change.
The figure shows the features produced by the optic mount at the top of the periscope before maintenance (red) and 3 hours after recovery from maintenance (blue). The amplitude seems reduced by nearly 10, but lets see how it ages. I used a watercolor paint brush to apply 5 minute epoxy to the base of the U-200 mount at the top of the periscope. I used one brush load. I was only able to paint the epoxy at the left and right sides of the mount because the middle was over a cutout in the base plate. After the epoxy was mostly cured, I adjusted weights on the periscope and optic, minimizing the peaks in IMC_F by placing them in valleys between periscope resonances.
Robert, Rick
Jordan, Sheila
In the summary pages, we can see that something non stationary appeared in DARM from about 80-250 Hz durring the long lock that spanned Oct 11th to 12th, and has stayed around. Links to the spectra from the 11th and the 12th.
HVETO also came up with a lot of glitches in this frequency span starting on the 12th, (here) which were not around before. These glitches are vetoed by things that seem like they could all be realted to corner statin ground motion: refl, IMC and AS WFS, all kinds of corner station seismic sensors, PEM accelerometers, MC suspensions.
Although this noise seems to have appeared durring a time when the microseism was high for us, I think it is not directly related. (high microseism started approximately on the 9th, 2 days before this noise appeared and things are quieting down now but we still have the non stationary noise sometimes up to 200 Hz.)
The blend switching could also seem like a culprit, but the blends were not switched at the begining of the lock in which this noise appeared, and we have been back on the normal (90mHz blends) today but we still have this noise. We've seen scattering from the OMC with velocities this high before (17264 and 19195).
Nutsinee and Robert have found that some of the glitches we are having today are due to RF45, but this doesn't seem to be the case on the 12th.
Robert, Sheila, Nutsinee
The first plot attached is a timeseries of DARM vs RF45 mod of the 10/11 - 10/12 lock stretch (~25 hours). The second plot is the same channels during the beginning of 10/13 lock stretch (30 minutes). You can see RF45 started to act up on 10/13. I've also attached the BLRMS plot of DARM using the bandpass filter Robert used to find the OMC scattering. The none stationary noise we see is likely caused by two different sources.
RF45 started to glitch Monday afternoon (16:04 PDT, 23:04 UTC). According to TJ's log no one was in the LVEA that day. The glitches stopped around 03:22 UTC (20:22 PDT)
Here is one example of one of these glitches rlated to ground motion in the corner that we had durring high microseim over the weekend (but not the entire time that we had high mircoseism). This is from Oct 12th at 14:26 UTC. Even though these have gone away, we are moitvated to look into them because as Jordan and Gabriele have both confirmed recently, the noise in the unexplained part of the spectrum (50-100 Hz) is non stationary even with the beam diverter closed. If the elevanted ground motion over the weekend madde this visible in DARM up to 250Hz, it is possible that with more normal ground motion this is lurking near our sensitivity from 50-100 Hz.
If you believe these are scattering shelves.
See josh's alogs about similar problems, especially 19195 and recently 22405
One more thing to notice is that at least in this example the upconversion is most visibe when the derivative of DARM (loop corrected) is large. This could just be because that is the time when the derivative of the ground motion is large.
Nairwita, Nutsinee
Nairwita pointed out to me that the non-stationary glitches we're looking at was vetoed nicely by HPI HAM2 L4C on October 12th, so I took a closer look. The first plot attached is an hour trend of DARM and HPI HAM2 L4C. But if I zoom into one of the glitches it seems to me that there's a delay in response between HPI and DARM up to ~10 seconds from just eye-balling it (second plot). I've also attached the spectrogram during that hour from the sumary page.
I ran Dan's code to compare stationarity between two hours on Oct 5th and Oct 12th. The closure of the beam diverter on the 6th was thought to help stationarity in the 70-100hz region, so I included versions zoomed in on that frequency range.
I tried to pick times that were not affected by huge glitches / range drops. On the 5th the two hours were 1:00-3:00UTC and on the 12th 00:00-02:00UTC.
plots attached
Sheila, Jordan
Made the same plots to compare the stationarity during times when anthropogenic seismic was quiet / loud. The 1-3 and 3-10 hz seismic bands pick up around 14:00 utc weekdays, and the data seems to become more nonstationary in the 100-200 Hz band during this time.
On the 12th, there is some unknown stuff going on at lower frequencies, and the ~300 hz periscope peaks are still visible. But just looking at the 100-200 hz region shows correlation with ground motion. Also have the same correlation on the 14th (spectrum overall looks very stationary, though). Mechanism still unknown... scattering?
TITLE: 10/13 EVE Shift: 23:00-07:00UTC (16:00-00:00PDT), all times posted in UTC
STATE of H1: In Observation Mode at 75Mpc
Outgoing Operator: Jim
Support: Occupied Control Room, Usual Suspects
Quick Summary:
Jim's computer crashed so he lost his log of activities for his shift. He did not have much to pass on other than being out for ~8hrs for Maintenance Day and recently getting H1 back up to Observation Mode. Off-topic, but he also showed me how to transition the ISI Stage-1 Blend Filters for high useism conditions (there's an actual sticky note on the Ops Work station about this.).
Richard, Jeff, Evan
It had been on for at least several months.
Darkhan T., Travis S.
During today's maintenance period, we took PCal calibration measurements for both end stations. Attached are photos of the datasheets (mostly for our own reference). Analysis of the data to follow.
Added 205ml cooling water to the TCSX chiller. First water added to TCSX in the past month. Added 600ml cooling water to the TCSY chiller. Given the amount of water loss with the TCSY Chiller but not with the TCSX Chiller over the past three weeks, I am suspicious there is a leak in the TCSY cooling loop. I added marks (at 1/4 , 1/2, and 3/4) next to the site glass so we can more easily track water loss.
and has been continually since Monday afternoon at ~39hz (1150rpm [19hz] at motor/pump.) Let me know if this is a problem.
I have disabled the IMC WFS offsets that Keita and Cheryl wanted to remove (alog 22370).
This may help the recent ISS issue (alog 22449) somewhat, but probably not a lot.
Background
I was investigating why the ISS recently started having the trouble in engaging the 2nd loop. A first thing I noticed is relatively high RIN after the IMC. It seems that the IMC adds some extra RIN below 1 Hz as the light goes through it. A large RIN at low frequencies can easily hinder the PID control of the 2nd loop when engaging. So this seemed suspicious to me.
Since the ISS 2nd loop had been running without a significant issue in the past, perhaps until the recent change on the IMC WFS (alog 22362), I speculated that the current IMC alignment is at a non-optimal point where the low frequency RIN became worse. One factor which affects the IMC alignment is the WFS offsets that are meant to minimize the jitter-to-RIN couplings. In the end, I decided to get rid of the offsets because it gave a better RIN coupling.
IMC_LOCK guardian edited
To disable the offset, I have commented out lines 555 and 556 in the IMC_LOCK guardian. They are now,
#ezca.switch('IMC-DOF_2_P', 'OFFSET', 'ON')
#ezca.switch('IMC-DOF_1_Y', 'OFFSET', 'ON')
RIN is better without the offsets
I did a simple test where I measured RIN after the IMC with and without the WFS offsets. Note that the offsets have been applied only on DOF2_P and DOF1_Y. They have not yet been optimized after the change in the IMC WFS. The measured RIN are shown in the attached screenshot.
Blue: RIN at the ISS in-vac array without the offsets, Cyan: RIN at the ISS in-vac array with the offsets, Brown and red: RIN before the IMC with and without the offsets, respectively. The 1st loop was always ON while the 2nd loop was always OFF. The input power was about 2 W.
First of all, it is clear that RIN after the IMC is higher than that before the IMC by a factor of more than 10 at around 0.1 Hz. I am not sure how long it has been like this.
Next, as shown in the plot, removing the offsets reduced the excess RIN below 1 Hz somewhat at the in-vac ISS array. This was repeatable and therefore I think the improvement is real. Additionally, it got rid of a nasty structure at around 600 Hz. Also, some peaks above 100 Hz decreased their peak heights by a factor of few. These improvements were consistenly observed at IMC-MC2_TRANS_SUM as well. Therefore I think they are real improvement in RIN and not some kind of spurious couplings such as spatial jitter.
So overall, the configuration without the offsets seems better in terms of RIN. Perhaps this is an indication of better WFS sensing. I decided to disable the offsets in the IMC_LOCK guardian. I did not try to optimize the offsets yet. So this can be a next action item.
SDFs are updated so as to accept the no-offset configurations in ASCIMC.
J. Kissel, S. Dwyer
While prepping for the PSL incursion today, we had supposed that we should offload DC values the IMC WFS CTRL OUTPUT to the IMC SUS's alignment sliders, a.k.a. "offload the MC WFS." This process has been historically dubious because there have been many MCWFS offloading scripts in various states of completion / testing, and the request to run the script from the IMC_WFS_MASTER MEDM screen does not tell you what script it is running, nor gives any indication that it has run or finished.
Today we've made this better.
We've
- Removed
${userapps}/release/ioo/h1/scripts/imc/mcwfsrelieve
${userapps}/release/ioo/common/scripts/mcwfsrelieve.py
from the svn repo.
- Edited
${userapps}/release/asc/common/scripts/imc/offloadMCWFS.py
to display text indicating the progress of the script as it goes (and committed to the userapps repo)
- Edited
${userapps}/release/asc/common/medm/imc/IMC_WFS_MASTER.adl
to call the offload script using xterm, such that a terminal pops up and displays standard out, i.e. the call to run the script in MEDM is now
xterm -g 140x10 -hold -e $(USERAPPS)/asc/common/scripts/imc/offloadMCWFS.py
- We've also edited the script to round off to the 10000th of a count (five decimal places), such that one can accept new offsets into any SDF system without having to worry about the precision problems that SDF has with small numbers.
We've successfully run the script 3 times, so we're sure that functional.
You should now call the offloading of WFS from the IMC_WFS_MASTER screen, as circled in red in the first screenshot. You should then see an xterm window pop up, and it'll walk through its processes -- see second attachment.
All of this infrastructure (as indicated by the paths) is common infrastructure that has now been committed to the repo. As such, LLO, needs only to update the screen and script to absorb the new goodness.
Due to oscialltions in the X arm IR loop that were causing difficulties in inital alingment, (22443), we made a small change to the Xarm locking filters today (WP#5558).
There was a pole at 100 Hz that did not make much sense, we moved it to a kHz now, which gives us an extra 40 degrees at the ugf of 100 Hz. Before and after rms and transfer function screenshots are attached. This should solve the egregious problem with the 1206 Hz instability, but there are still problems with the loop, which due to the distribution filters in MC2. These distribution filters are used in MCL, ALS COMM and CARM loops, so we will not try to fix these today.
First, note that the rms of M2 and M3 are both dominated by things below 0.5 Hz, meaning that we need a boost in the top stage. We could probably skip M2 altogether as we have done with the recycling mirrors. Also, Evan and Jeff note that the loop is rather flat around 100 Hz, which is because of a 41z:150p in MC2 M3.
[Jeff K, Duncan M]
With Jeff's assistance (and that of the on-duty operator) I have remotely updated the EPICS configuration for ODC to commission the state monitoring for the new PINJX infrastructure [alog 22445 22465 22470 22473].
Changes were made to EPICS records in the h1calex, h1iscex, and h1odcmaster models as follows
These changes have been monitored and accepted in SDF for the relevant models and can serve as a reference for L1 when the same changes are made next week.
Associated changes were made to the ODC MEDM screens in order to show the CAL_X ODC input. This required separating the SYS_CUST_ODC_MASTER_END.adl screen into separate screens for MASTER_X and MASTER_Y (no CAL_Y ODC). These changes were committed to userapps as r11886.
Added H1:SUS-SR3_M2_TEST_P_OFFSET to the exclude list and rescanned. Added 70 channel names. Removed 11 channel names. All except H1:SUS-SR3_M2_TEST_P_OFFSET were H1:CAL channels.
Over the last few days, we've been trying out the new 45 mHz blend filters for the BSC ISIs, which are designed to help out during times of high microseism.
This aLog is just meant to be a collection of logs relating to the switching, to help Team DetChar know which state things were in at which times, so they can hopefully make a comparison. One of the things that might be most interesting is the effect on the artifacts that Josh pointed out in aLog 22405.
Some of the logs that have talked about the switching back and forth include aLog 22440 and aLog 22459.
Looking at the SWSTAT of the ISI-[chamber]_ST1_BLND_[x or y]_CPS_CUR_SWSTAT channels I can see when the blends were in each state. FM7 is the nominal 90mHz blends (SWSTAT = 40000), and FM9 is the new 45mHz blend (SWSTAT = 40192). Below is a table of the lock stretches in each state.
| 90 mHz blends (nominal) | 45 mHz blends (new) |
| all locks through the one ending 10 Oct, 21:25 UTC | |
| 11 Oct 16:22 UTC - 12 Oct 18:11 UTC | |
| 13 Oct 00:53 UTC - 13 Oct 09:30 UTC | |
| 13 Oct 11:35 UTC - 13 Oct 14:43 UTC |
For some background, 45 mHz blends provide us with isolation at the microseism, which may be partially coherent between the buildings. When we lock with 90 mHz blends, we lock the position of the ISI to stage 0 at the microseism frequencies. With the normal seismic environment at LHO we find this better, because the interial sensors confuse wind induced building tilt with translation at these frequencies and if we try to use them to isolate they move the ISI in response to these spuirious signals.
In the fall, we tend to have less wind and more microseism, meaning that our seismic environment can sometimes be more similar to LLO's normal situation. Using the 45 mHz blends which are more similar to LLO's had allowed us to lock durring a high microseism, low wind time when we were unable to lock on our normal 90 mHz blends. We know that durring winds above about 20 mph we will be imposing spurious tilt signals on the ISI with these 45 mHz blends, which can make locking imposible or difficult.
So can you tell us the impact of these blends on DARM by comparing lock stretches with similar microseism and wind but different blends? It would be good to know this for a few different environmental conditions, (say winds below 15 mph and microseism high, and winds from 15-30 mph and microseism high).
I've rearranged the PRMI branch in the DRMI guardian, and added states to the ISC_LOCK guardian to request both these states and the ALIGN_IFO states used for PRMI (finshing unfinished item from WP5533). This is for use when you think that the DRMI alignment is bad (based on the AS camera and the flashes as seen in dataviewer) and will not lock. If DRMI is slow to lock but has been locked recently and looks well aligned on the AS camera, this procedure is probably not your best bet.
We will test this durring maintence recovery today, but the instructions replacing those in 21745 will be:
done!
This has now been tested, and had some bugs but after fixing several typos we made a sucsesfull transition from PRMI to DRMI. If you are trying to lock DRMI and decide to change to PRMI, you would need to take ISC_LOCK to manual, then request LOCK_PRMI, and go back to AUTO.
And remember "Manual" will be on the "ALL" screen for ISC_LOCK (it's the pink button on the upper left). [I forgot where this button was and had to call Sheila!]
On Tuesday, while most of the IFO was down for various maintenance tasks, I grabbed a bunch of SUS spectra and started a Template directory.
I set all of the references to be the ~quiet, unlocked data from the down period of the IFO. These spectra could be run when trying to troubleshoot locking. On Tuesday, I was only able to collect the following, located in /ligo/home/ops/Templates/SUS_Spectra/
BS_NOISEMON_spectra.xml
BS_OSEMINF_spectra.xml
PR2_NOISEMON_spectra.xml
PR2_OSEMINF_spectra.xml
PRM_NOISEMON_spectra.xml
PRM_OSEMINF_spectra.xm
SR3_NOISEMON_spectra.xml
SR3_OSEMINF_spectra.xml
SR2_NOISEMON_spectra.xml
SR2_OSEMINF_spectra.xml
SRM_NOISEMON_spectra.xml
SRM_OSEMINF_spectra.xml
ITMX_NOISEMON_spectra.xml
ITMX_OSEMINF_spectra.xml
ITMY_NOISEMON_spectra.xml
ITMY_OSEMINF_spectra.xml
NOTE - Many of the lower stage NOISEMON channels look... weird. They should be used as a before/.after snapshot for troubleshooting only. Work to improve what the various strangenesses of these channels is on a few low priority to-do lists.
There are templates ready to collect the balance of the SUS spectra data, namely ETMs, MCs, PR3. We should do this when the IFO is set to DOWN for whatever reason. The spectra are quick to run, then update all references (currently bogus data) and resave.
While we were unlocked due to wind during my Sunday Owl shift, I managed to get through taking, updating, and resaving templates for:
ETMX_NOISEMON_spectra.xml
ETMX_OSEMINF_spectra.xml
ETMY_NOISEMON_spectra.xml
ETMY_OSEMINF_spectra.xml
PR3_NOISEMON_spectra.xml
PR3_OSEMINF_spectra.xml
We set all quadrant gains of IMC WFSA to [1 1 1 1] from [1, 0.25, 1, 4]. (WFSB was already all 1.)
We also disabled IMCWFS error offsets in servo filters.
After this, we steered IM2 to bring the beam position on IM4 trans back (at first we tried IM3, but it would make the OSEM output to become larger, and they're already close to saturation).
IFO locked after this without any problem.
We haven't done any jitter coupling optimization and I don't know if Robert had time to do it.
The first and the second attachment show the current and the old settings, respectively.
In the first one, yellow boxes show what we changed. Red box show what we changed but are somehow reverted (automatically?).
This is just an observation related to entry 22482 where I was investigating the relation between ISS and IMC.
After Keita and Cheryl set the IMC WFS gains back to 1, it seems to have shifted the pointing to the ISS array a little bit. See the attached trend.
The QPD signals at the ISS array have moved by 0.1 or so both in PIT and YAW when the WFS gain was changed to 1. Both PIT and YAW moved towards the center of the QPD although SUM seems to have decreased at the same time. I am not sure what exactly was going on. We may need to optimize the pico-motors to minimize the jitter-coupling to the ISS array.