The beam tube cleaning was restarted last week, 02/19/2016, with the same Apollo crew that was on site previously. Scott L. and Ed P. Beginning at Mid-Y and working towards the corner after getting things set up again, the crew was able to clean 163 meters of tube ending 9.14 meters east of HSW-1-092. This included vacuuming out the support tubes and capping them in those sections.
1540 - 1605 hrs. local -> To and from Y-mid Next fill will be Wednesday, Jan. 27th before 4:00 pm
Title: 1/25 Shift 16:00-24:00 UTC (8:00-16:00 PST). All times in UTC.
State of H1: Locked at DC Readout for Commissioning measurements
Shift Summary: After tweaking up IMs, I was able to get Input_Align to lock long enough to offload the alignments. Since then we have had several locklosses due to SDF reversions and MC2 saturations. The IFO has come up quickly and easily after each lockloss.
Incoming operator: Jim
Activity log:
15:45 Chris to X end area for beam tube sealing
16:07 reset ITMx WDs that were tripped upon arrival
17:08 Jeff B to optics lab
17:38 Mitchell to optics lab
17:48 Jeff B out
17:52 Mitchell out
18:05 locked NLN
18:15 lockloss due to SDF reversion
18:30 Joe D to X arm beam tube sealing
19:00 Karen to MY
19:14 Karen done
19:29 lockloss MCS saturation?
20:00 Joe D back
20:06 locked NLN
22:19 lockloss unknown cause
23:15 locked DC readout for Jenne's measurments
23:17 beam tube crew done
23:30 Betsy to optics lab
23:42 Betsy out
23:46 Kyle and John to MY
According to the cross-spectrum technique (alog 25039), L1 has a different characteristic in noises from 40 to 200 Hz. No surprise.
While a H1 spectrum shows somewhat-feature-less 1/f noise with a sharp 60 Hz peak and its harmonics, L1 seems to have extra structures including a few broad bumps in 50-150 Hz. See the attached plot below.
I picked a GPS time of 1131307217 (Nov 11 2015 20:00:00 UTC) for the L1 spectrum. This is a period well before the L1 dropped the inspiral range and seemingly less non-stationary in 10-200 Hz.
The ASD parameters are the same as those for H1 -- Hanning, 50% overlap, 1 Hz bandwidth for a 12 minutes data chunk. I used the DARM model of the L1 calibration group to calibrate the cross-spectrum. I have not corrected the time-varying parameters (i.e. kappas) for this analysis. I have not subtracted thermal noises.
We have had plenty of things wrong in the IFO since we used bad safe.snaps to restore after the power outage last wensday. (A2L gains, missing ASC notches, ETMY bias was accidentally flipped, plenty of dark offsets changed, some violin damping was on with the wrong filters engaged ect...)
This morning Jenne, Kiwamu and Evan helped me to clean this up so we are nearly back in the observe state from O1, with only intentional changes like the LSC feedforward and sending MICH to PR2, which we have accepted.
There are a few things remaining red:
The bias is flipped on ETMY, and the gain in L3 DRIVEALIGN_L2L (which compensates for the bias flip). It might be that we have messed up the calibration by doing this flip accidentally, but we were planning on doing it soon anyway.
I've also implemented a version of the scripts from LLO that load down.snaps in SDF when the IFO goes down, and observe.snaps when we reach nominal low noise. So far we only have saved a few down.snaps, but if we add more and keep them up to date this should be alot easier in the future since we won't need to be locked to see what differences we have.
After the IFO lost lock Jenne, Trais and I went through SDF and updated the downs that I had made last week after the power outage, and made down.snaps for the models that had differences from the observe state. I also added these the the bash scripts that the guardian uses to load sdf files.
We also flipped the bias on ETMY back.
This means that if we loose lock from nominal low noise, SDF should be all grey and green now. If we loose lock from a different state (like we just did during the CARM offset reduction) SDF will not be green.
Now if we can keep these up to date we can avoid this kind of trouble in the future. We probably need to think about how we are going to keep these up. Maybe it can be a weekly maintence task?
I have cleared the rest of the SDF diffs that we have for today in the Observe state.
For some reason, SR2's setpoint had the M2 Pit and Yaw inputs turned off. This isn't right, so I've accepted the correct state of having the inputs turned on so the signal can go through.
I have also accepted the gain of -1 in the PR2 ISCINF_L filter bank, which is used for the PRCL-MICH decoupling as of last week.
The last thing I accepted was a filter module turned on in the SRM's ISCINF bank that Gabriele created to try to get rid of the 3.2kHz broad peak in DARM that is very very coherent with SRCL.
We're still taking measurements right now, but SDF is green, so we should be able to leave the IFO in Observe when I'm done.
Laser Status:
SysStat is good
Front End power is 29.79W (should be around 30 W)
Frontend Watch is GREEN
HPO Watch is RED
PMC:
It has been locked 5.0 days, 1.0 hr 36.0 minutes (should be days/weeks)
Reflected power is 1.822Watts and PowerSum = 23.85Watts.
FSS:
It has been locked for 0.0 days 0.0 h and 3.0 min (should be days/weeks)
TPD[V] = 1.432V (min 0.9V)
ISS:
The diffracted power is around 8.727% (should be 5-9%)
Last saturation event was 0.0 days 0.0 hours and 2.0 minutes ago (should be days/weeks)
Other than work permits, the morning meeting consisted primarily of Tuesday maintenance planning. Items for Tues. maintenance include:
Aidan here (next week?) for TCS work
Dave O, Elli, and new student here for HWS work
Peter gave us notice of a 2W NPRO running in the staging building triples lab. Signage and barriers are up.
Hugh will also be taking the SEI system down to check the HEPI Fluid side Accumulator pressures--couples hours for the CS at least.
The X1 DTS has been restarted with the exception of the frame writer and NDS. The LDAS gateway computer seems reluctant to boot, and is required for the frame writer and NDS.
no restarts reported for both days.
There are small glitches very close to each second boundary in the ETMY drive signal and the ETMY SUS ad SEI rack magnetometers. In order to investigate the half-Hz combs in DARM (see alog 20790), I took an hour of data and folded it with a four-second period. If there is a repeated glitch at any multiple of this period, it should become far more visible. The result is that in several channels, there are glitches very near the boundary of each GPS second. The peak time of these glitches seems to be about 10 milliseconds after the start of the second. The glitch does not repeat identically every second. There is one shape in the first second, then one with an opposite polarity in the next second. The first two attached plots are for the SUS and SEI racks, which are shown with a 40-Hz zero-phase lowpass. The SUS has a narrow spike, and the negative spike is larger than the positive one. The SEI signal is more complicated. The ETMY L3 MASTER signal, which is the DARM output to the ESD, is shown with a 10 to 50 Hz bandpass. These glitches are more like sine-Gaussians, but the even and odd seconds still seem to have opposite polarities. There are more channels with similar glitches. We can make a more thorough investigation, and use more data and more times, to try to track down the origin of these glitches. Hopefully these glitches are responsible for the 0.5 Hz combs such that removing them will improve those.
J. Kissel Tagging CDS in this entry. I'd recently taken a look at the requested output of the ETMY L1 stage, ${IFO}:SUS-ETMY_L1_MASTER_OUT_*_DQ and was interested to find ~1 [Hz] combs in the requested output. Though this isn't the 0.5 [Hz] combs that Andy mentions above, I think it's an excellent place to take the investigation further in a more focused manner -- with the point being that even the SUS's *requested* signal has a comb. Attached is a 100-sec FFT ASD, of a typical, 1000 [sec] stretch of observation-ready data during the run (2016-01-04 04:00 UTC). Here, to give a feel for the physical amplitude of these signals: at 30 [Hz] the noise amplitude of one of these comb peaks is roughly 1e-3 [ct/rtHz] of requested DAC output, which corresponds to 1e-3 [ct/rtHz] * (20.0 [V] /2**18 [ct]) = 7.6e-8 [V/rtHz] @ 30 Hz ( * sqrt(2 * 0.01) = 1.1e-08 [V_pk]) Potentially verifiable / refutable Crack-pot Theories / Wild guesses: - Perhaps there is some of this glitching in the inter-process communication (IPC) on the reflected memory (RFM) data transfer from the corner to the end station, that's only exposed for requested drives that have such a huge dynamic range? For whatever channels in the signal chain that are stored, can you reproduce the same combs by filtering those channels offline? - Recall that the power supplies for the Hartmann Wavefront Sensor (HWS) were replaced some time ago, see Integration Issue 1062. Has anyone made a before-and-after comparison on this searched other sources for such combs in auxiliary channels? Perhaps forming a BruCo-like search where this UIM / L1 stage control signal is the response instead of DARM? - Keith has already done a long-term study of the analog-to-digital converters (ADCs), looking for combs: see, eg. pg 44-49 (yeah!) of G1300997. He found no-such combs. Perhaps we should do a similar study on the digital-to-analog convert (DAC) side of things? I could also imagine a similar set up for a set of RFM channels that make the 4km journey along the arms.
In response to Jeff: The SUS-ETMY MASTER signal is just a filtered version of DARM, so if DARM has the comb so do the drive signals. I don't think that tells us where in the loop they originate. But you're right, this could be a digital problem or an electronics one involving something synched to GPS. Keith T. and Annamaria both suggested that the power supply of the timing fanout might be involved. That of course can be perfectly synched to the GPS second. Annamaria showed me an ADC in the L1 corner station being used as a temporary monitor of one of these power supplies. That signal (attached) jumps downward one second and upward the next, matching what we see in the magnetometers and DARM. Could we check if there's such an effect at the H1 Y-end?
Note that the small glitches in Andy's post are exactly synchronized to GPS; this makes coupling to many power supply glitches (HWS, or trickle chargers for magnetometers, etc.) an unlikely source.
An electromagnetic shaker on the blue cross beams of the BS chamber produced greater upconversion than was produced by shaking of any other chamber or the PSL table (ITMY wasn’t shaken) (https://alog.ligo-wa.caltech.edu/aLOG/index.php?callRep=24194). I unsuccessfully tried to reproduce this upconversion using stage 2 ISI injections in X, Y and Z (I did not try RX, RY or RZ). Next I investigated the upconversion by injecting single lines with the EM shaker on the BS cross beams in order to find the most sensitive frequency band. Figure 1 shows the line injections that produced the most upconversion; they are located between 40 and 65 Hz. Lines injected with amplitudes between 1 and 2 orders of magnitude greater than normal produced broad features around the injection frequency and at harmonics, with amplitudes that were several times background in DARM. The next step will be to inject uniform bands in order to estimate the contribution of the 40-65 Hz vibration background to the DARM noise in the 80-200 Hz band.
I spent some time looking at how we can reduce the DARM residual.
In the attached plot (template lives in evan.hall/Public/Templates/LSC/DarmResReduce_2015-01-23.xml), yellow shows the nominal DARM residual and estimated freerunning displacement.
Blue shows the residual after the addition of a 3 Hz resonant gain. I put this in LSC-DARM FM10, so the freerunning estimate should still be correct. [However, since the DARM filter bank is full, I had to overwrite some other filter. After this test was over, I reverted my changes and placed this RG filter in the LSC-OMC_DC filter bank for safekeeping.]
Red shows the residual after the addition of the 3 Hz resonant gain, as well as a microseism boost, which I put in LSC-OMC_DC. This affects the freerunning estimate, but the amplitude and phase changes at and above 10 Hz are minimal (less than 2 ° of phase change at 10 Hz).
Here is a plot similar to the one in 25053.
It shows the DCPD spectra from last saturday when I had a 6 Hz line injected, with the predicted upconversion from the DC readout quadratic term explaining the line at 12 Hz as well as the noise in the DCPDs at around 10 Hz. The red trace is the spectrum evan calls nominal above, where there were no changes to the DARM loop but the feed forward was retuned, as you can see the predicted upconversion is reduced by nearly 2 orders of magnitude at 10 Hz, and the upconversion around the calibration lines is reduced.
The black trace is once Evan had added both a boost and a resonant gain to the DARM loop, so we expect the DCPD specrtum to be reduced at low frqeuency simply because of the change in the DARM loop shape. You can see that there is also a reduction in the predicted upconversion around the calibration lines as well as at 10 Hz.
Incidentally I was looking at the residual spectra of LLO and LHO (from Jan 1 2016 00:00:00 UTC) for some other reason. I post the plot for the record.
I ran BruCo on one hour of data from last night. The report is available here:
https://ldas-jobs.ligo.caltech.edu/~gabriele.vajente/bruco_1137640217/
At low frequency, SRCL and DHARD_P are the largest contributions. SRCL is still a factor of few below the measured noise, while DHARD is very close around 14 Hz.
There is coherence with magnetometers (still far from the measured noise)
No significant broadband coherence in the mistery noise region.
Aborting a DTT measurement caused a lockloss - no good, although not a new phenomenon.
Since there are so many SDF diffs, I'm wouldn't put the IFO in Observe anyway, so I'm going to just leave it Down for the night.
Reported as FRS Ticket 4274, so we begin to quantify how often and how painfully this remaining DTT abort problem affects us.
We noticed a small bump in DARM at about 360 Hz, coherent with PRCL. We added a 270-430 Hz elliptic band-stop. DARM improved and the coherence is almost gone. We are losing 9 degrees of phase at 50 Hz (PRCL UGF).
The filter is implemented in the SUS filter bank.
The bandstop filter is now engaged by the guardian in the NOISE_TUNING step.
Kiwamu, Sudarshan
ISS Outer Loop Servo Board (S1400214) was modified to include a zero at 100 Hz to obtain a better phase margin. This was done by replacing a resistor R74 from 0 Ohm to 154 Ohm (D1300439) and has been documneted in the E-traveler.
Initial test has been done after the modification and the board will be installed today during the maintenanace period. Further performance test will be done after the installation and with loop closed.
The second loop transfer function measurement was taken after the modifications were done. The plot and data is attached.
ISS Inner Loop has UGF of 22 KHz with a phase margin of about 50 degress. This was measured with variable gain set at 6 dB for the best phase margin. This is the normal operation settings for Inner Loop.
Outer Loop has a UGF of 1 KHz ( designed for 4 KHz) with a phase margin of about 30 degrees. The variable gain was set at 40 dB (max available) and an additional gain stage(?) was switched on as well.
Also tried moving the the Inner loop gain to see if it shows any improvement on the outer loop but no luck.
TF Plots are attached.
These transfer function measurements were taken at ~10 W of PSL power.
The data used for the plot above is attached.