Looking over the past 3 weeks of data for the Laser Room temperature, the attached plot shows 4 deviations from the norm. The first two coincide with maintenance activities carried out by Jason and myself. The third from the left by Cheryl and Robert doing some IO work. The fourth one from the activity this week. Each incursion results in a change in the pre-modecleaner body temperature with perhaps the largest change occuring this week. Since most times we probably touch up the pre-modecleaner alignment a little, this probably masked the effect of the pre-modecleaner body length change on the alignment.
This is a follow up to this entry about the excess noise in the EX TR QPD signals. The OSEM fix did not help this, so they seem to be unrelated. I looked at the PIT and YAW signals, and found that they are very coherent with SUM in the 5-100 Hz band where the excess noise appears (plot 1), and that the phase of the transfer function in that region is 0 (e.g., SUM, PIT and YAW all have the same sign and phase). This appears to point to a problem in segment 1, though I cannot confirm that with offline data. I looked at the OUT16 channels for all segment and didn't see anything obviously wrong (plot 2). Interestingly, the same signal appears in QPD A and B, so this is not a single channel problem.
To do: investige the individual segment signal in the online data... is this just sement 1?
Most of the night IFO was with commissioners.
Earthquake about 2 hours ago kept us from relocking for a while.
IFO has made it through to Engage ASC a few times, so transition to CARM is ok.
I've been having the IFO sit in Engage ASC, which I thought was very stable, but it has not been this morning, and we have not had any locks that are long or that make it up to DC Readout+.
The main story of the day is related to the non stationary low frequency noise first seen early in the morning. It seems to come from CHARD noise, which could be coupling to DARM more now because of a change in alignment.
A few ideas for next steps:
We also worked on a few other things today...
Here is a measurement of CHARD Yaw at high power, overlaid with yesterday's measurements at 23W. The 23W measurement includes the MsBoost, but not any 23W boost or the lead-plus-cutoff filters that Sheila designed.
Here is how I retuned the A2L. I injected some band limited noise (ellip band pass 1-100 Hz, amplitude 20000 cts) on ETMX_L2 L2L, P2P and Y2Y paths, with the P2L and Y2L gains set to zero. The measurements were good between 20 and 100 Hz. The ratios -P2P/L2L and -Y2Y/L2L are what we need to implement in the correction paths. Those trasnfer functions are quite constant above 30 Hz, but not so much below 30 Hz. We would need a better (sweep sine) measurement if we want to improve the decoupling below 20 Hz.
I changed the gains of the P2L and Y2L of ETMX as follows:
P2L from 1.18 to 1.03
Y2L from 1.33 to 1.23
Coherence of DARM with CHARD reduced at low frequency. However, we reverted to the old numbers to investigate the low frequency non stationary noise.
I ran Hang's latest A2L script (see aLog 20013), after the realignment work that was done tonight (Sheila is writing up her entry as I type).
We stil have excess noise at low frequency, but maybe there's a bit less than when I started the script? The noise we're seeing is totally non-stationary, so it's hard to say. Certainly the A2L didn't eliminate it.
I checked the results of the latest a2l run. It seemed that the decoupling worked only for ETMX pitch and ITMX pitch, and the optimal gains changed only by 7% and 2%. On the other hand, it failed for ETMY pitch and ITMX yaw. I attached a worked result and a failed one for comparison.
By examining the results, the bad ones had a flatter slope and were more likely to have "outliers". We thus might be able to get a better result by increasing the steps between two measurements, or increase the number of gains to be measured. Nonetheless, it seemed to also indicate that we were already near the optimal spot that such an linear, single frequecy decoupling could achieve...
Dan, Nutsinee
Tonight we identified and damped more ITM first harmonics.
| Frequency | Test Mass | Damp Setting |
| 991.7478 | ITMY | 260dB, -60deg |
| 991.9345 | ITMY | 260dB, 120deg |
| 992.4256 | ITMX | 260dB, +/-180deg |
| 997.8868 | ITMY | 260dB, +/-180deg |
They will be added to the violin wikipage.
All Times in UTC
(Dan, Corey)
Around 5:30UTC (22:50PT), Dan noticed a rung up roll mode on DARM spectrum, and from the Bounce/Roll monitor, the culprit was ITMy.
Brought up the bounceroll.stp StripTool from the Ops Template & could see ITMroll channel high. From the ITMy SUS screen, opened the DARM BR DAMP filter bank screen.
Initial Values: -60degrees & a gain of +40.
New Values: +60degrees & a gain of -80.
This took care of ITMy, and should be fine for this current lock. Whether we want to keep ITMy like this remains to be seen. Should see how we look after a few locks.
After the PSL temperature adventure on monday afternoon, it seems as though the PMC alignment shifted. We now get less transmitted power, although the sum of refl and trans has not changed much.
In looking at the data around the period of the temperature excursion, all the power monitoring photodiodes indicate a change in power monitored. The ones located before the pre-modecleaner return to their previous values. The ISS photodiodes after the pre-modecleaner return to their previous values however the transmission and reflection signals are lower than before. The pre-modecleaner reflected spot doesn't look substantially different, however the pre-modecleaner heater output did not return to its previous level. It has remained at an elevated level since the temperature excursion. The coefficient of thermal expansion for aluminium is approximately 22 microns per degK. The attached plot suggests the body of the pre-modecleaner changed by 0.5 degK and stayed at the higher temperature. It should be noted that the pre-modecleaner heater did its job and relieved the PZT high voltage. In doing so the length of the spacer is different and this may be the cause of any mis-alignment. The plot also shows the Laser Room temperature. It might be worth trying reducing (presumably reducing, might also be increasing) the heater offset to bring the pre-modecleaner temperature back down to 304.5 degK from its current value of 305.0 degK to see if this peaks the power transmitted by the pre-modecleaner.
Attached is the output of the quadrant photodiode in the ISS photodiode box with the corresponding temperature measurement. Clearly a change in the beam position is indicated, with the vertical not returning to its previous value. The horizontal seems to track the room temperature.
FRS 3247 The h1hwinj0 computer has been renamed to h1hwinj2.
Scott L. Ed P. Rodney H. 8/11/15 After filling the water tank, the crew moved the fans and re-strung the lights. 45 meters of tube and bellows were cleaned ending at station HSW-2-012. Cleaning results posted here. 8/12/15 60.6 meters of tube and bellows cleaned ending at station HSW-2-009.
Sheila, Elli
Summary:
Yesterday morning durng maintenance we went out quickly to measure the beam parameter ar AS-Air. IThe beam waist is 3.7e-4 (1e-4) m at the AS_Air camera. The fit of the beam divergence is pretty bad, we were hurrying to get done quickly and I didn't take enough data points to get a good fit for the beam divergence. Using measured waist size and the (very poor) fit of beam divergence, the beam parameter at the AS_AIR camera is calculated to be 0.14+0.22i in the vertical axis and 0.16+0.29i in the horizontal axis. UPDATE: Today during the Earthquake at lunchtime I went out and took some more measurement points. I am fitting these new points at the moment, and hopefully they will improve this measurement.
Details:
We used a straight shot through corner station with PRM, ITMX, SRM misaligned. We placed a flipper mirror 0.434m upstream of the AS_Air camera, which sends the AS-Air beam across ISCT6 where we used a Thorlabs BP-104 slit scanning beam profiler to measure the beam profile at 5 locations (see optical layout diagram). This beam scanner is mounted on its side, so that Y is the horizontal axis and X is the vertical axis. The laser power was turned up to 24W to get enough light on Thorlabs beamscan to take a measurment (and the backgorund noise was still high at 24W).
The background noise was to high for the beam profiler to automatically fit beam waist, so we saved the beam shape in the x and y axes and fitted a waist size to these beam profiles after the measurement was over. Puzzlingly, the maximum intensaity in the X and the Y directions is not the same.The fit of the gaussian beam in x and y is good. Then plotted beam radius vsd distance to fit the waist location and size with a hyperbolic function. There aren't enough points/too much error in each point to get a satisfying fit. I have attached a fit which looks kind of reasonable, but really there is too much variation in the points to call this a good fit .(See picture of alternative fit which is almost as good, and very different.) So the Beam waist location/size can't be pinned down using this meaurement. This measurement could be inproved by taking more data points.
The ALS end station shutters have temporarily been commented out of the guardian. (They will no longer close, even in the shuttered state). The goal is to have green light locked in the arms while we are at a good sensitivty, with the idea that this could possibily be helpfull for determining if some of the glitches we see are due to dust. ( alogs 20395 20355 20328 )
We had originally added the closing of the shutters since we heard that it improved the noise at LLO, even though we saw no evidence that it improved our noise here. After a few weeks of engineering run we should revert this change.
Reset the dust monitor alarm levels for the LVEA, VEAs, and PSL from the tighter levels associated with the June vents to the levels for the O1 environment. The current values are:
| Room Air | Size | Minor Alarm | Major Alarm |
|---|---|---|---|
| 0.3-Microns | 14,000 | 20,000 | |
| 0.5-Microns | 7,000 | 10,000 |
| Anti & Laser Room | Size | Minor Alarm | Major Alarm |
|---|---|---|---|
| 0.3-Microns | 1,400 | 2,000 | |
| 0.5-Microns | 700 | 1,000 |
The Diode Room and Optics Lab alarm levels will be adjusted when I can get confirmation of their particle level requirements
Set the Diode Room alarms to the same Clean-1000 levels as the PSL.
Some random commissioning tasks from tonight:
LSC rephasing
In full lock, the phases of POP9 and POP45 were adjusted to minimize the appearance of PRCL in POP9Q and the appearance of SRCL in POP45Q. Then the input matrix element for POP9I→SRCL was tuned to minimize the appearance of a PRCL excitation in the SRCL error signal. New settings attached.
We should take a sensing matrix measurement sometime soon.
LSC OLTFs
I took OLTFs of PRCL, MICH, and SRCL. The data are attached.
[I also did some noise injections into CARM for frequency budgeting purposes. Those are attached too.]
Front-end LSC triggering
Jamie and I started this a few weeks ago, and now it is completed.
There are occasions when the DOWN state of the ISC_LOCK guardian (which, among other things, turns off feedback to the suspensions) is not run immediately after a lockloss (e.g., because the guardian is paused or in manual mode). Therefore, Jamie and I set up the LSC trigger matrix so that PRCL, MICH, SRCL, DARM, and MCL are turned off if POP DC goes below 100 normalized counts. This is set in the DRMI_ON_POP state.
CARM gain redistribution in the Guardian
The state REFL_IN_VACUO now redistributes the CARM gain slightly in order to improve the noise performance of the CARM loop. This state has not been tested and has been left commented out.
The CARM gain code was uncommented and seems to work fine.