TITLE: 07/28 Owl Shift: 07:00-15:00 UTC (00:00-08:00 PST), all times posted in UTC
STATE of H1: Observing at 54Mpc
OUTGOING OPERATOR: Ed
CURRENT ENVIRONMENT:
Wind: 7mph Gusts, 5mph 5min avg
Primary useism: 0.01 μm/s
Secondary useism: 0.05 μm/s
(4) EQs seen in the last 24hrs, but now the winds have just died down and useism is still low.
QUICK SUMMARY:
Current lock is almost 5hrs long.
I walked toward the Control Room to the howls of coyotes just before midnight; they didn't return my howls.
Sheila, with many conversations with Keita, Jeff K, and others
We have several reasons to believe that something changed in our suspensions durring the Montana EQ. (See alog from Beverly Berger and Josh Smith, (37775) which got us started looking at this, and Cheyl's log about the large triples, (37674). We are still looking at some of the data from alignment sensors, but here arer some things we can say:
There is more to be done checked on here, for example, checking if this has happened at any other times during the run (I checked one large EQ, I see no shifts like this), checking yaw (which has much smaller shifts than pitch), checking the triples, and looking at the alignments of the reaction chains. Can we interpret the information we have to make a gues aout what might have changed in the suspension? Wire slipping or some kind of damage to the prisms are some things we have been thinking about.
Hysteresis is a possibility here. We discovered on the LASTI quad during one of the early builds that these suspensions have significant hysteresis in pitch. That is, if you tip the stages a given amount, they will not come back all the way, leaving you with a pitch offset. The attached plot shows a measurement of this effect from LASTI, showing a pretty standard looking hysteresis plot. We learned that you can 'undo' any offsets by getting the pendulum swinging, and letting it slowly damp itself. The slower the ringdown, the closer it returns to its nominal 'equilibrium' position.
The offsets you see here don't look any bigger than what we saw there, though granted we were trying to measure the effect, so pushed it pretty far. Then again, we didn't have any major earthquakes either.
There were many documents written to investigate what we saw at LASTI. Mark Barton's document, T0900103, includes a list of most if not all of them.
So it could be that this earthquake induced some hysteresis offset, or perhaps there was an offset already and the swinging motion from the earthquake removed it. Anyway, try swinging the pendulum in pitch with some large *but safe* amplitude, and you should return to the nominal 'equilibrium' position, if it isn't already there.
Looking at Beverly log (37775) that shows DC changes in the pitch offset across the earthquake time. Are the changes in the pitch in the lower masses compatible with the reported change at the top mass?
Here are some additional plots, for those who are interested in what happens to the osems between the reaction mass and the top mass. I also have plots that show torque applied to the reaction mass vs measured pitch, these aren't very useful because we don't change the torque applied to the reaction mass, but they do show that there were similar shifts in the reaction chain. In order to interpret the data from the L1 and L2 osems we will need to account for shifts in the reaction chain.
Posting a jpeg version of the LASTI hysteresis plot above, since the pdf was causing issues.
Also, here is a summary of the procedure I used to make the plot way back in 2008:
"These data points are separate pushes and releases. The procedure was to put the top mass on its stops with the rest of the chain suspended. Note, the quad was on the test stand outside the chamber at the time. Then the top mass stops were used to tip the top mass some amount in pitch. The angle of the test mass, with the top mass still tipped, was measured with either an autocollimator or optical lever. That test mass angle is the X axis in the plot, called ‘Input Pitch’. Then the top mass was released slowly to avoid oscillation, and the test mass pitch angle was recorded again. That value is the Y axis, called ‘Output pitch’. This process was repeated for successively larger and larger Input pitch values, until I was afraid to tip the suspension any more. I then started to tip the suspension in the other direction until I was again afraid to tip the suspension any more. And finally, to close the hysteresis loop, I repeated some of the data points along the original tipping direction."
6:53UTC INJ_TRANS node active. LLO acknowledged.
06:23UTC As per Sudarshan's aLog, I changed the calibration line configuration. Below is an image of the SDF diffs accepted to go back into Observing.
All BS spectra look fine. ETMY shows the only slightly elevated HF noise. Nothing to be concerned with.
All HAM spectra looks good.
Violin modes.
We are running two Pcal lines at ENDX at 333.9 and 1083.3 Hz with amplitudes twice as large as yesterday to get better SNRs. These lines will be on for two hours. The SDF changes as a result of changing the amplitudes were accepted and monitored. Ed will turn these lines off in two hours and start a high frequency line at 3001.3 Hz.
It was a little more than two hours. See my aLog.
~01:00UTC It didn't report this afternoon.
J. Kissel I'm behind on my documentation as I slow process all the data that I'm collecting these days. This aLOG is to document that on this past Tuesday (2017-07-25) I took standard top-to-top mass transfer functions for the Triple SUS (BS, HLTS, and HSTS; 10 SUS in total), as I've done for the QUADs (see LHO aLOG 37689 and associated comments). I saw no evidence of rubbing during the act of measurement, but I'd like to confirm with a thorough comparison. As such, I'll post comparisons against previous measurements, other suspensions, and the appropriate model in due time. This leaves: 3 doubles, 9 singles. Data is stored and committed here: /ligo/svncommon/SusSVN/sus/trunk/BSFM/H1/BS/SAGM1/Data/ 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_L_0p01to50Hz.xml 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_P_0p01to50Hz.xml 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_R_0p01to50Hz.xml 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_T_0p01to50Hz.xml 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_V_0p01to50Hz.xml 2017-07-25_1501_H1SUSBS_M1_WhiteNoise_Y_0p01to50Hz.xml /ligo/svncommon/SusSVN/sus/trunk/HLTS/H1/PR3/SAGM1/Data/ 2017-07-25_1507_H1SUSPR3_WhiteNoise_L_0p01to50Hz.xml 2017-07-25_1507_H1SUSPR3_WhiteNoise_P_0p01to50Hz.xml 2017-07-25_1507_H1SUSPR3_WhiteNoise_R_0p01to50Hz.xml 2017-07-25_1507_H1SUSPR3_WhiteNoise_T_0p01to50Hz.xml 2017-07-25_1507_H1SUSPR3_WhiteNoise_V_0p01to50Hz.xml 2017-07-25_1507_H1SUSPR3_WhiteNoise_Y_0p01to50Hz.xml /ligo/svncommon/SusSVN/sus/trunk/HLTS/H1/SR3/SAGM1/Data/ 2017-07-25_H1SUSSR3_M1_WhiteNoise_L_0p01to50Hz.xml 2017-07-25_H1SUSSR3_M1_WhiteNoise_P_0p01to50Hz.xml 2017-07-25_H1SUSSR3_M1_WhiteNoise_R_0p01to50Hz.xml 2017-07-25_H1SUSSR3_M1_WhiteNoise_T_0p01to50Hz.xml 2017-07-25_H1SUSSR3_M1_WhiteNoise_V_0p01to50Hz.xml 2017-07-25_H1SUSSR3_M1_WhiteNoise_Y_0p01to50Hz.xml /ligo/svncommon/SusSVN/sus/trunk/HSTS/H1/ PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_L_0p01to50Hz.xml PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_P_0p01to50Hz.xml PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_R_0p01to50Hz.xml PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_T_0p01to50Hz.xml PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_V_0p01to50Hz.xml PR2/SAGM1/Data/2017-07-25_1607_H1SUSPR2_M1_WhiteNoise_Y_0p01to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_L_0p03to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_P_0p01to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_R_0p01to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_T_0p01to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_V_0p01to50Hz.xml PRM/SAGM1/Data/2017-07-25_1607_H1SUSPRM_M1_WhiteNoise_Y_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_L_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_P_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_R_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_T_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_V_0p01to50Hz.xml SR2/SAGM1/Data/2017-07-25_1715_H1SUSSR2_M1_WhiteNoise_Y_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_L_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_P_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_R_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_T_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_V_0p01to50Hz.xml SRM/SAGM1/Data/2017-07-25_1814_H1SUSSRM_M1_WhiteNoise_Y_0p01to50Hz.xml
More detailed plots of BS, compared against previous measurements and model. We see perfect agreement with model and previous measurement, so this SUS is definitely clear of rubbing.
More detailed plots if PR3 and SR3. Both are clear of rubbing. The new measurements agree with old measurements of the same suspension, the model, and other suspensions of its type. PR3's L2L transfer function shows "extra" unmodeled resonances that were not there before, but they line up directly with the Y modes. This is likely that, during the measurement the Y modes got rung up, and the power is so large that it surpasses the balance the of the sensors, so they're not subtracted well. I can confirm that these frequencies are incoherent with the excitation, and we've seen such inconsequential cross coupling before. Nothing about which to be alarmed.
More detailed plots of PRM, SRM, and SR2 compared against previous measurements and model. We see good agreement with model and previous measurement, so these SUS are clear of rubbing. There is a subtle drop in response scale factor for all of these suspensions (and in retrospect it's seen on the other SUS types too), and I suspect this is a result of the OSEMs LEDs slowly loosing current over the series of measurements, see attached 4 year trends.
While PR2 shows all resonances are in the right place, there is a suspicious drop in scale for the L and Y DOFs with respect to prior measurements. However, this is the first measurement where we've measured the response with the nominal alignment offsets needed to run the IFO (!!). These DOFs (L and Y) have the LF and RT OSEM sensor / actuators in common (see E1100109 for top mass OSEM layout), so I checked the OSEM sensors, an indeed the LF OSEM sensor is on the very edge of its range at ~1400 [ct] out of 32000 (or 15000 [ct] if it were perfectly centered). I'll confirm that the suspension is free and OK tomorrow by retaking the measurements at a variety of alignment offsets. I really do suspect we're OK, and the measurement is just pushing the OSEM flag past its "closed light" voltage and the excitation is becoming non-linear, therefore reducing the linear response. I attach the transfer function data and a 4 year trend of the LF and RT OSEM values to show that we've been operating like this for years, and there's been no significan change after the Jul 6th EQ.
I'd forgotten to post about the OMCS data I took on 2017-07-25 as well.
The data lives here:
/ligo/svncommon/SusSVN/sus/trunk/OMCS/H1/OMC/SAGM1/Data/
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_L_0p02to50Hz.xml
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_P_0p02to50Hz.xml
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_R_0p02to50Hz.xml
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_T_0p02to50Hz.xml
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_V_0p02to50Hz.xml
2017-07-25_1812_H1SUSOMC_M1_WhiteNoise_Y_0p02to50Hz.xml
Detailed plots now attached, and they show that OMC is clear of rubbing; the data looks as it has for past few years, and what difference we see between LHO and LLO are the lower-stage Pitch modes which are arbitrarily influence by ISC electronics cabling running down the chain (as we see for the reaction masses on the QUADs).
The C00 vs. C01 comparison pages have been updated and include all C01 data between 2016-11-30 0:00 and 2017-06-20 0:00.
As part of this analysis, I've got updated PCAL-to-DARM ratio trends at 36.7, 331.9 and 1083.7 Hz. Plots of both magntidue and phase residual timeseries trends are attached. As a reminder, these trends are computed by demodulating 300-second segments at each PCAL line frequency, then averaging to get a magnitude and phase out of each channel. In practice, I break up each 300-second segment into overlapping 100-second chunks, apply a Kaiser window, and then average over chunks to get a less noisy measurement. (It's basically Welch's method, except I'm demodulating rather than computing a PSD.) Finally, I remove outliers that are due to locklosses and loud transient glitches.
In each plot below I show PCAL/strain trends for C00 (blue) and C01 (red) data. The trend shown in aquamarine applies a correction for f_cc to C01 data at the appropriate PCAL line frequency. Gray shaded regions correspond to times when we had a break in O2, once during the holiday season and once for commissioning work. This is identical to a similar study done on Livingston data; see L1 aLog 35102.
You can see that in the bucket (331.9 Hz) we continue to have no systematics and only very small (~1%) statistical fluctuation when we correct for f_cc. At high frequency (1083.7 Hz) there's a slight systematic offset in magnitude and phase, but it's at the level of 2% or so which is consistent with Craig's error budget. At low frequency (36.7 Hz) there's a 3-4% systematic offset since we came back after the break on June 8 that isn't accounted for by f_cc, but I'll bet it's due to optical spring detuning. The offset also shows up in ASD ratio spectra; see the DetChar summary page from the first day after break. I have it as an action item to look into this in the next few days, so stay tuned!
I have restarted SegGener_H1 to include the H1:DMT-ITMY_L2_DAC_OVERFLOW as defined by TJ. This shouldn't have any side effects other than a loss of 1-2 secons of segment data. The H1 IFO was not in low noise data taking at the time so this shouldn't matter much.
John reported via email this change was successful on the production machine, but the DMT test machine hung (probably for other reasons) when he was testing the change. I've now power cycled h1dmt3, and it is up again. This completes LHO WP 7094.
I think I have the seismon code running a bit better now. At least it is running on it's own, and hasn't needed restarting since last week. The main differences are now the 5 event epics code looks like its running, and the seismon_run_info script I'm using now touches on the current event folder every loop. I think this was getting "cleaned up" before and not getting recreated or something. I've added a test to diag main if any earthquake has an arrival time in the future, so there is at least some notification that an earthquake is coming. This should be in addition to the verbal test (which may need updated? I'm not sure what TJ has done) that also has a threshold on the predicted ground velocities. The earthquake today was below the verbal threshold, so didn't get noticed by verbal alarms, but seismon gave us plenty of warning.
TITLE: 07/27 Eve Shift: 23:00-07:00 UTC (16:00-00:00 PST), all times posted in UTC
STATE of H1: Earthquake
OUTGOING OPERATOR: Jim
CURRENT ENVIRONMENT:
Wind: 15mph Gusts, 12mph 5min avg
Primary useism: 0.05 μm/s
Secondary useism: 0.06 μm/s
QUICK SUMMARY:
Observatory mode was put into "Environment-EQ" after the earthquake. Since then we've made it to NLN but not for very long. I'm leaving it in "Environment until we get re-locked with stable range.
J. Kissel, J. Warner We've lost lock due to a non-exciting earthquake, re-acquired up to DC Readout Transition watching the violin modes carefully, but we lost lock there (while sill controlling DARM with ETMX). Upon the *next* re-acquisition, though, the ETMX violin modes were incredibly rung up. As such, we stopped at Shutter ALS and baby-sat the ETMX modes until the DCPD RMS was reduced from 1e4 to 2e3. We used Ed Merilh's as our babysitter configuration for the now-problematic ETMX MODE 4 at 505.805 Hz, namely driving in Length, Pitch, and Yaw, ~75 gain, FMs 1 (505.805), 2 (-60 deg), and 4 (100dB). This was successful, so we've now programmed this into the guardian. We highly recommend operators hold any re-acquisition from now on at SHUTTER_ALS, wait for the OMC to lock, then grab a ~0.005 mHz spectra, and opening the outputs of ETMX first 5 violin MODE filters to make sure that violin modes are not rung up. Then, if violins are OK (i.e. RMS of DCPDs is less that 2e3 [ct]), you can go to the first Violin Mode Damping state but be prepared to turn the damping filters off before things get terrible! Only one more month of this, team -- we can do it!
It may be that the violins are so rung up that you're saturating AS_C, which makes SRC2 loop unstable -- so you'll see pitch go into slow oscillation. To prevent this, after every lock loss (for now), park the IFO in ENGAGE_REFL_POP_WFS, and run a DTT spectra with the following channels. H1:OMC-DCPD_A_IN1 H1:OMC-DCPD_B_IN1 H1:ASC-AS_C_SEG1_IN1 H1:ASC-AS_C_SEG2_IN1 H1:ASC-AS_C_SEG3_IN1 H1:ASC-AS_C_SEG4_IN1 To move past ENGAGE_REFL_POP_WFS, you need the AS_C segments to have an RMS of ~2000 [ct] or less below the 500 Hz violin mode cluster, and all peaks should be below 20000 [ct/rtHz]. Once that's true, you can move on the turn on the automatic violin mode damping as normal, so select VIOLIN_MODE_DAMPING_1. To move past that, it's the same criteria: and RMS of ~2000 [ct] or less below the 500 Hz violin mode cluster, and all peaks should be below 20000 [ct/rtHz]. It won't be until you get an RMS of ~100 [ct] RMS that you'll stop seeing huge shoulders around the lines, so *keep baby sitting*.
Templates can't be attached 'cause they're too big. Look in /ligo/home/jeffrey.kissel/Templates/ H1ASC_AS_C_forViolins.xml H1DCPDs_forViolins.xml
Just performed an OSB walkthrough, nothing to report.
Seismon-5-Event: