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Reports until 12:26, Friday 21 October 2016
H1 ISC (ISC, TCS)
aidan.brooks@LIGO.ORG - posted 12:26, Friday 21 October 2016 - last comment - 23:19, Friday 21 October 2016(30718)
TEM10 HOM mode appears to be ringing up around 5kHz. [YARM?]

Summary:

There is a broad peak in the DARM spectrum around 5kHz which is consistent with the TEM10 being rung up at that frequency. 

Details:

The attached MATLAB file produces an animation that shows the DARM spectrum around 4700 - 5500 Hz. It updates this spectrum for 50s intervals around the time that the IFO is locked. Very quickly we see a broad peak (around 50Hz wide) form in DARM around 4900 Hz. This peak moves up in frequency as the lock is maintained.

I have the online simulation of the HOM spacing (frequency vs time) shown in the top plot. As the anmation steps forward in time, we can start to find the maxima of the broad peak in DARM. I've taken the location of these maxima and plotted them in the FREQ vs TIME plot (I've only picked the location of the maximum value of the broad peak and tried to exclude all times before the lock is acquired and the frequency starts to change). The transient behaviour is quite consistent with what the simulation predicts. 

The two figures correspond to two recent locks but different ETMY ring heater settings:

  1. GPS TIME: 1160974817: ETMY RH = 0W
  2. GPS TIME: 1161055457: ETMY RH = 1.1W (aLOG 30685)

After the ETMY ring heater is turned on and stabilizes, we expect the HOM frequency to shift down by about 60Hz, according to the simulation. We see a commensurate change in the location of the peak in DARM.

If this is the TEM10 mode in the arm, then what is ringing it up?

 

 

 

Time 2:

 

 

More to come ...

(Download and run the MATLAB file to see the animation).

Images attached to this report
Non-image files attached to this report
Comments related to this report
terra.hardwick@LIGO.ORG - 23:19, Friday 21 October 2016 (30743)

TEM10 mode overlaps with 47.5 kHz mechanical modes (see here) which we see aliased down around 18050 Hz. We have two PI in ETMY (47495 Hz and 47477 Hz) which ring up strongly during the beginning of the lock (through the first hour), which would of course ring up TEM10 in turn. 47495 Hz broke the second lock time you look at after about an hour. I'll run your matlab file over the weekend and compare to the amplitude behavior of these PI. (Also note that the ETMY ring heater change you mention was specifically to move into a zone where there's more overlap with these mechanical modes so that I could check our ESD damping capabilities.)

H1 CDS (DAQ)
david.barker@LIGO.ORG - posted 12:25, Friday 21 October 2016 (30720)
CDS model and DAQ restart report, Wednesday 19th, Thursday 20th October 2016

model restarts logged for Thu 20/Oct/2016 No restarts reported

model restarts logged for Wed 19/Oct/2016
2016_10_19 09:33 h1fw0
2016_10_19 10:13 h1fw0
2016_10_19 10:22 h1fw0

2016_10_19 10:59 h1fw0

Unexpected fw0 restarts, logs indicate slow file system access problems. Power cycled h1ldasgw0 (not shown) and h1fw0. No subsequent restarts as of time of this alog (49+ hours).

H1 PSL
peter.king@LIGO.ORG - posted 12:15, Friday 21 October 2016 (30719)
modified pre-modecleaner servo
Made a small modification to a pre-modecleaner servo that reduced the boost gain by
lowering its corner frequency.  Installed the servo and couldn't lock the pre-modecleaner.
After about ~15 minutes of trying, I gave up.  The original pre-modecleaner servo was
re-installed.  With it I noticed on the CCD camera that the alignment had shifted.
Re-aligned the beam into the pre-modecleaner, checked alignment onto the locking
photodiode, re-locked the pre-modecleaner.
LHO VE
kyle.ryan@LIGO.ORG - posted 10:14, Friday 21 October 2016 (30716)
~0900 hrs. local -> Measured X-end RGA temperatures - made incremental adjustments
Bake of RGA is going good thus far, still "inching" toward 180C < temperatures < 200C everywhere excepting the tapering-off to 90C at turbo inlet.
LHO General
patrick.thomas@LIGO.ORG - posted 08:40, Friday 21 October 2016 (30715)
Ops Owl Shift Summary
Lock loss at NLN, same as last night, DHARD pitch went into oscillation. Since Terra only needed high power and not NLN, stopped there for subsequent locks.

07:10 UTC Sheila to LVEA to check PSL enclosure air conditioning
07:15 UTC Sheila back
07:28 UTC Attempting to lock
08:00 UTC Stopping at INCREASE_POWER (50W) for Kiwamu and Sheila
08:26 UTC Moving to NLN
08:32 UTC NLN
08:36 UTC Lock loss
08:53 UTC PRMI to DRMI transition worked
09:06 UTC Lock loss almost immediately upon reaching DC_READOUT
09:12 UTC I'm trying to turn off the ISS autolock, but something keeps turning it back on.
09:41 UTC DC_READOUT. Waiting for roll modes to damp.
09:49 UTC Moving on
10:01 UTC NLN
10:05 UTC Lock loss. DHARD oscillation before hand.
10:10 UTC Turning off ISS autolock turns on the first loop integrator? Turning on the ISS autolock turns off the first loop integrator?
10:30 UTC Stopping at INCREASE_POWER (50W). Terra taking PI measurements.
11:00 UTC Lock loss (PI mode 27)
11:21 UTC Stopping at INCREASE_POWER (50W). Terra taking PI measurements.
12:10 UTC Lock loss (PI mode 27)
12:14 UTC IR not found for diff. Found by hand.
12:34 UTC Lock loss just after reaching DRMI_LOCKED.
13:00 UTC Stopping at INCREASE_POWER (50W). Terra taking PI measurements.
14:16 UTC Changed ITMY ring heater upper and lower requested power from 1.25 W to .25 W per Terra's request.
14:23 UTC ETMY violin mode 9 rang up. Terra changed the damping gain to damp it.
15:03 UTC Lock loss. Trouble locking PRMI. Catches but does not hold.
H1 AOS
terra.hardwick@LIGO.ORG - posted 08:37, Friday 21 October 2016 (30710)
47495 Hz mode controllable with OMC DCPD signal

Summary: ETMY PI 18041 Hz - aliased down from 47495 Hz, Mode27 - is (more readily) dampable if the OMC DCPD is used as error signal.  ESDs provide adequade force if actuating on mode while it is < 4 orders of magnitude above OMC-PI_DCPD noise floor (~10^4 magnitude in OMC-PI_DCPD channel), ~2.5 orders of magnitude above QPD noise floor.  

- - -

Previously we had been unable to damp Mode27 (alog 29685) and turned off ETMY ring heater (alog 29702) to have less optical mode overlap with this 47495 Hz mechanical mode. Wednesday night I turned the ETMY ring heater back on to revert back to the bad zone and more thoroughly test our ESD damping capabilities. This mode has the highest gain during the transient time.

Over the past 20 hours and about 10 locks, I've found we have the actuation force to damp this mode if it is caught early ( < 4.5 orders of magnitude above noise floor in OMC signal ) which is much more likely when using the OMC DCPDs. All PI damping nominally uses error signal from TransMon QPDs. The OMC DCPDs also see mechanical modes and with an SNR ~15x the QPDs (see here for example from tonight of Mode27 seen in both error signal paths). We have avoided using DCPDs as error signal becaues the coupling path is not well understood and we see gain sign flips and much less steady phase changes. However, the high SNR seems necessary for PI with high gain that rings up quickly so that the damping loop can actuate against it more immediately while the mechanical mode amplitudes are still lower. This and other PI in the 47kHz ring up especially quickly (and twice) during the first hour transient sweep. Mode is very responsive and easily damped with a gain sign or phase change under 4 orders of mag above noise floor (1k magnitude in H1:OMC-PI_DCPD_64KHZ_AHF_DQ); above 4 is gets less responsive and is essentially non responsive by 5 (10k mag). So while we do have an error signal from QPDs within the effective damping range, the smaller window combined with high PI gain/rapid ring ups make the QPD signal inadequate. 

Operators: I've left Mode27 in the new OMC DCPD scheme. Patrick and I found a pattern of needing to change the gain sign twice during the beginning of the lock and adjust phase after that during the next hour or so. This mode responds very quickly, so be ready to immediately revert gain signs if it turns out to be the wrong direction. 

Note: Rang up with single quadrants (LL or UR) a few times and saw slightly less effective actuation than with LL+UR, though still need to process actual ring up time constants to compare effect. I switched once to LR, UL drive but many modes went crazy and broke lock so didn't try again tonight. Will repeat at lower power to get relative quadrant coupling for a given mode. 

Images attached to this report
H1 PSL
peter.king@LIGO.ORG - posted 08:30, Friday 21 October 2016 (30714)
NPRO trend data
NPRO pump diode output power and NPRO output power for the past 12 months.  The power decay for the pump diodes
has more or less levelled out.  We no longer really have any margin left for the pump diodes.  At this stage of
their life, increasing the diode current might precipitate their demise.

    The NPRO power may have levelled off too.  We should still plan on replacing the NPRO during the mid-run
break.
Images attached to this report
H1 ISC
terra.hardwick@LIGO.ORG - posted 08:00, Friday 21 October 2016 (30713)
4735 Hz

We had the 4735 Hz violin mode ring up bigly ~13:30 UTC. Was able to damp by flipping the sign; it's still fairly rung up so incoming operator should keep an eye. This is ETMY MODE 9.

H1 ISC
terra.hardwick@LIGO.ORG - posted 07:18, Friday 21 October 2016 - last comment - 10:37, Friday 21 October 2016(30712)
ITMY ring heater turned down

Per Sheila's request, we just reduced ITMY ring heater 1.25 W --> 0.25 top, 1.25 --> 0.25 bottom at 14:16 UTC.

Comments related to this report
kiwamu.izumi@LIGO.ORG - 10:37, Friday 21 October 2016 (30717)

The CO2 settings were also reverted to the values that we used to use before the ring heater tuning started. Here is a summary.

  • Cold state values [CO2X CO2Y] = [0.5, 1.0] Watts => [0.5, 0.3] Watts
  • Hot state values [CO2X, CO2Y] = [0.24, 0] Watts => [0.2, 0] Watts

To implement this change, I have edited the following guardians.

  • ISC_LOCK
  • TCS_ITMY_CO2_PWR

I did not get a chance to check the contrast defect in the simple Michelson configuration yet.

H1 PSL (ISC, PSL)
sheila.dwyer@LIGO.ORG - posted 01:54, Friday 21 October 2016 - last comment - 22:16, Sunday 23 October 2016(30708)
Another look at DBB injecting noise into DARM

Keita, Sheila, Kiwamu

This afternoon Keita and I did another test of opening and closing DBB shutters, since Keita realized that there are multiple shutters that matter.  The results are in the screen shot.  We only see two shutters on the PSL layout, (SH01 in the 35 W path to the DBB and SH02 in the 200W path) and on the photos documenting the table, but there must be a third shutter, perhaps inside the DBB box. We did not test switching to the 35W beam because that caused a lockloss last night. Apparently the shutters used here are Thorlabs SH05, which has an aluminum blade according the the thorlabs website. 

When changing between shutter states today we saw a broad band change in the DARM noise throughout our 200Hz-1kHz lump, (this is a little different from what we saw last night).  However, we saw 3 different noise states in DARM depending on the shutter requests, shown in the attachment.  

  shutter open shutter closed
no beam worst best 

200 W

intermediate worst

We guess that the shutter which is controlled by the epics channel "PSL-DBB_SHUTTER_DBB" is inside the DBB box itself and not on the layout.  It is hard to explain the table above.  For example, if no beam is selected, and both beams are really blocked before they reach the DBB, why would closing the shutter inside the DBB matter?  

Kiwmau and I went inside the PSL, placed beam dumps in the paths to the DBB.  We placed a "black hole" beam dump (no cone in the middle) in the HPO path (a 250 mW beam between M3 and M12 on the layout).  Looking at that beam with an IR card, we could see a corona around it, pictures will be attached to this alog.  This corona is scattered around, hitting the black baffle near the DBB apperature and other things.  We also placed a black glass beam dump upstream of the front end laser beam path the the DBB, just before the shutter. 

Update:

After waiting out the Japanese earthquake, we relocked.  The lump was smaller in the first moments of the lock.  After a few minutes the peaks reappeared, but the peaks still changed when we opened and closed the shutters, in a way that is repeatable although the plot is confusing since the overall level of noise was changing probably with the thermal state.  (each time we opened the shutter, things got worse than they had been).

We do not understand how changing the shutter state impacts the DARM noise, although we think we have ruled out scattered light.   Kiwamu thought that perhaps the change in the noise could be due to the change in the diffracted power when we move the shutter (see Keita's alog 30679). We tried a test of changing the diffracted power, which unlocked the IFO.  It could also be through the same electrical coupling that means the diffracted power changes when we open the shutter. 

Images attached to this report
Comments related to this report
peter.king@LIGO.ORG - 06:29, Friday 21 October 2016 (30711)
One consequence of these table layout modifications is that we've lost the signal that monitors the output
of the high power oscillator.
sheila.dwyer@LIGO.ORG - 18:19, Friday 21 October 2016 (30735)

Keita suggested that one non optical way that shutter states could impact DARM is if somehow the shutters move more when open than closed.  I had a look at accelerometers on the PSL table (table 1).  There is coherence of around 0.3 between this accelerometer and DARM at the frqeuency of the peaks which depend on the shutter state.  However, there was no difference in the coherence or the spectrum of the accelerometer when the shutters were open.  It seems unlikely this is a mechanical coupling. 

Also, The second attachment shows a trend of the power out of the PSL as we changed the shutters (DBB_SHUTTER controls SH01 and SH02, the two that are outside the DBB, 0 is both closed 1 is 200W beam open; DBB_SHUTTER_DBB is the one that must be inside the DBB box itself.)  The two shutters we switched both reduced the output power by about 1.5Watts, and the impact is additive (both shutters closed is about twice as much power lost as either one of the shutter closed.)

However, as shown in the plot in the original post the noise impact is not additive, both shutters open is slightly less noisy than either single shutter open.  

Images attached to this comment
sheila.dwyer@LIGO.ORG - 22:16, Sunday 23 October 2016 (30777)

I didn't add the attachment to the above alog showing the power out of the PSL change as we opened and closed shutters on the DBB.

Here is one, which shows both the ISS diffraction changing, and a laser power monitor

Images attached to this comment
H1 General
nutsinee.kijbunchoo@LIGO.ORG - posted 23:28, Thursday 20 October 2016 (30709)
Ops EVE shift summary

TITLE: 10/20 Eve Shift: 23:00-07:00 UTC (16:00-00:00 PST), all times posted in UTC
STATE of H1: Down. Earthquake.
INCOMING OPERATOR: Patrick
SHIFT SUMMARY: Been stopping at Increase Power so far. Couple of locklosses. One was due to 9.32Hz rung up (DHARD loop related) and one due to PI mode27 (18043Hz) rung up really fast.

LOG:

01:18 Lockloss -- 9.32Hz rung up

04:05 Kiwamu and Sheila to PSL

04:25 Lockloss -- PI rung up (fast). Was able to find the right phase where the mode became stablized but it was too late.

05:34 Unable to lock due to a 6.2M earthquake in Japan. Take IFO to Down.

H1 ISC (ISC)
jenne.driggers@LIGO.ORG - posted 18:00, Thursday 20 October 2016 (30706)
10W should see the lump if it exists

[Stefan, Jenne]

We looked at the cross-power spectrum at 10W and at 50W, to see if we would be able to see the smooth "lump" at several hundred Hz if we do as PeterK suggests and lock with 10W, no HPO on Monday.

Our conclusion is that at least at the beginning of a 10W lock, the answer is no lump.  While the shot noise makes it difficult to see whether the lump is there or not, by taking a long cross power spectrum (DCPD_A vs. DCPD_B) we can dig down much deeper. 

In the attached screenshot, we show the 50W and 10W calibrated DARM spectra (labeled "asd"), the shot noise level assuming the spectrum is shot noise limited at 1340Hz ("shot") and the cross-power-spectra calibrated to amplitude units ("cross-asd").  Note that the 10W shot noise almost limits our ability to see the lump, but the cross-asd tells us that the lump isn't there.  The 10W spectra are taken with 15,000 averages, while the 50W spectra is only 1,500 averages.  10W data is from 20:56:00utc today, while the 50W is from our best time last night around 06:44:00utc. 

We'll look more at the data later, but we are currently back at 10W, and at the beginning it looked like the lump was there (spectra and quick cross-power-spectra), but 10 min later it is starting to go away.  This is definitely something thermal-related, and not relating to the different amount of polarization we let through the rotation stage + PBS. 

Images attached to this report
H1 General
jim.warner@LIGO.ORG - posted 15:58, Thursday 20 October 2016 (30704)
Day Shift Summary

TITLE: 10/18 Day Shift: 15:00-23:00 UTC (16:00-00:00 PST), all times posted in UTC
STATE of H1: Locked at Increase Power

SHIFT SUMMARY: Locking was mostly fine today. Needed some care at DRMI acquisition after high power locklosses, otherwise PI was PI

Few people went to mid stations, Peter did a test of PSL make up air, otherwise no other work done in VEAs.

H1 OpsInfo
terra.hardwick@LIGO.ORG - posted 15:13, Thursday 20 October 2016 (30703)
PI StripTools

PI StripTool on nuc6 now has two StripTools. Upper StripTool (PI_monitoring.stp) handles modes with frequency under 17k Hz, lower (PI2_monitoring.stp) with frequency above 17kHz.

We've seen more modes than fit on a single StripTool and with the upcoming TCS changes, it's probably best to keep an eye on all possibilities. Both StripTools are found in /opt/rtcds/userapps/release/isc/h1/scripts and can be opened from the PI Overview medm screen. 

H1 ISC
stefan.ballmer@LIGO.ORG - posted 14:41, Thursday 20 October 2016 - last comment - 14:57, Thursday 20 October 2016(30701)
Minutes commissioning meeting 2016/10/20

Reports: 

- DBB shutter open results in a huge noise bump issue

- peaks are smaller, but still there wtih DBB closed off

- PMC high voltage noise: (HV drive coherent, better readout--> peaks visible, realignment of PMC improved peaks / but hump is still there)

- coupling mechanism from PMC length offset to DARM unclear

- PMC UGF was 600Hz instead of 5kHz. going to (nominal) 5kHz made DARM noise worse.

- Reducing PMC loop gain further is not helping enough

- projection ~x2 below noise bump.

- PMC wrong polsarization light? (would be almost resonant, and therefore sensitive to PMC length noise) not clear how the coupling downstream of PMC works.

- Jitter spectrum looks smooth - thermally diven? Is so, other modes also produced... 20 mode...!

 

- picomotor steering into PMC to test...

- SRM: alignment affects jitter bump... !?

======================================================================

To do:

- 9MHz missing in reflection (x5 missing: (2W-50W we are loosing 2.5x)) - > find 1W of 9MHz (what was the conclusion for REFL9 gain?) 

- Low noise operaion at 12W, 24W (available in guardian)

- ER9 TCS configuration?

- PMC pole down

- Donut jitter verification? How?

 

Things to copy from LLO:

- Black glass for ETM camera to eliminate back-scatter

- ESD bias noise / zero crossing * run with ESD offset /reduced bias

- Compensation plate alignment ?

- PCAL switch (too much noise?)

 

"classical" tunings to be redone at operating point:

- A2L / ASC tuning

 -Aux loops feed-forward

=======================================================================

Timeline:

- HPO: Earliest: Monday 10/24

        - Option: 12W low power test first

- ER10 start LLO Oct 31 / LHO 10 days later

========================================================================

Comments related to this report
keita.kawabe@LIGO.ORG - 14:57, Thursday 20 October 2016 (30702)

Another to-do that was discussed: Make-up air on/off test when IFO is locked.

H1 ISC
terra.hardwick@LIGO.ORG - posted 14:05, Thursday 20 October 2016 - last comment - 18:58, Thursday 20 October 2016(30698)
New ITMY PI 18136 Hz

Lockloss ~19:30 UTC was due to rapid rise (about 10 min into 50W) of new ITMY PI at 18136 Hz. It's now become MODE24 and was damped the following lock with the PLL scheme. 

First saw mode in the live broadband monitor (found on PI medm screen under the StripTool button). I identified the arm by looking at SUS-ETMX/Y_PI_DOWNCONV_DC2_SIG_OUT_DQ spectrum at time right before lockloss. I identified test mass by alternating matrix elements to send damping signal to ETMY (with no result) then ITMY. Screenshot of PLL, broadband monitor, and StripTools during successful damping are attached. 

Images attached to this report
Comments related to this report
terra.hardwick@LIGO.ORG - 18:58, Thursday 20 October 2016 (30707)

Another new PI at ETMX 17771 Hz, now MODE7.

Belongs to the Xarm though test mass is unknown so far. Rang up about 2 hours into 50W lock (five orders of mag above noise floor in OMC DCPD) and rang down on it's own before I noticed it. I set up damping scheme in MODE7 and its been added to StripTool.

H1 CDS
david.barker@LIGO.ORG - posted 14:04, Thursday 20 October 2016 - last comment - 16:22, Thursday 20 October 2016(30699)
Status of front end simulink model files at LHO

Here is a table showing the current LHO simulink mdl files which have local modifications not checked into svn and/or have pending updates from the svn repository.

Note that the SUS MASTER common files are currently incompatible with the H1 sus models and should not be updated until we are ready to apply Stuart's changes.

file local mods? pending updates from repository comments
sus/common MC_MASTER.mdl no YES  
sus/common OMCS_MASTER.mdl no YES  
sus/common HSSS_MASTER.mdl no YES  
sus/common HSTS_MASTER.mdl no YES  
sus/common  HLTS_MASTER.mdl no YES  
sus/common SIXOSEM_F_STAGE_MASTER.mdl no YES  
sus/common BSFM_MASTER.mdl no YES  
sus/common PI_MASTER.mdl YES YES possible conflict
sus/common TMTS_MASTER.mdl no YES  
sus/common QUAD_MASTER.mdl no YES  
sus/common QUAD_ITM_MASTER.mdl no YES  
sus/common SIXOSEM_T_STAGE_MASTER.mdl no YES  
asc/common IAL_LOCKIN.mdl no YES not used by any H1 model
isc/common LSC_TRIGGER.mdl no YES  
isc/common FILTBANK_TRIGGER.mdl no YES  
lsc/common lsc.mdl YES no DBB jitter FF?
lsc/h1 h1lsc.mdl YES no DBB jitter FF?
sys/common IWAVE.mdl no YES  
Comments related to this report
david.barker@LIGO.ORG - 16:22, Thursday 20 October 2016 (30705)

SUS MASTER files have been made read-only to prevent accidental updates

H1 ISC
sheila.dwyer@LIGO.ORG - posted 00:47, Wednesday 19 October 2016 - last comment - 15:59, Thursday 20 October 2016(30648)
PMC HV noise, TCS, and lump in DARM from 200-1000Hz

The first attached screenshot is a series of DCPD spectra from the last several months.  When we first turned on the HPO, the noise in DARM did not get any worse.  The noise stayed similar to O1 until July 16th, the lump from 200-1kHz started to appear in late July, when we started a series of changes in alignment and TCS to keep us stable with a decent recycling gain at 50 Watts.  

PMC

Last night, Gabriele pointed out that the noise in DARM is coherent with the PMC HV.  The HV readback had been mostly some white noise (probably ADC noise), until the last few weeks, but has been getting noisier so that some of the things jitter peaks show up in it now (SEcond attached screenshot, colors corespond to the dates in the DCPD spectrum legend.  This may be related to the problem described in LLO alogs 16186 and 15986.  The PMC transmision has been degrading since July, which could be a symptom of misalingment.  Since July, the REFL power has nearly doubled from 22 to 38 Watts, while the transmission has dropped 28%.  The PMC sum has also dropped by 4%, roughly consistent with the 3% drop in the power out of the laser.  Peter and Jason are planning on realigning the PMC in the morning, so it will be interesting to see if we see any difference in the HV readback.  

TCS + PRC alignment:

The other two main changes we have had in this time are changes in the alignment through the PRC, and changes to TCS.  These things were done to improve our recycling gain and stability without watching the noise impact carefully.  In July we were using no offsets in the POP A QPDs.  We started changing the offsets on August 1st, after the lumpy noise first appeared around July 22nd.  We have continued to change them every few weeks since then, but generally moving in the same direction.  

The only TCS change that directly coresponds to the dates when our noise got worse was the reduction of ETMY RH from 0.75 W each on July 22nd, the other main TCS changes happened September 10th.  It would be nice to undo some of these changes before turning off the HPO, even if it means reduing the power to be stable.  

Images attached to this report
Comments related to this report
daniel.sigg@LIGO.ORG - 07:26, Wednesday 19 October 2016 (30651)

The HVMon signal (PMC length) shows a peak at about 600Hz/rtHz. We don't this is an indication of frequency noise from the laser, but rather an error point offset picked up in the PMC PDH signal. As such this is length noise added to the PMC and suppressed by the cavity storage time. Assuming this factor is about 1/10000, we would still get ~100mHz/rtHz which are modulated onto the laser frequency. Seems a lot.

The HVMon measure 1/50 of the voltage send to the PZT. With no whitening this is not very sensitive.

daniel.sigg@LIGO.ORG - 11:02, Wednesday 19 October 2016 (30659)

After the PSL team adjusted the PMC alignment the ~400Hz peaks are no longer visible in the HVMon spectrum. The coherence is gone as well—except for the 1kHz peak.

Non-image files attached to this comment
sheila.dwyer@LIGO.ORG - 16:38, Wednesday 19 October 2016 (30672)

About the PMC:

1st screenshot  shows the small improvement in DARM we got after the PMC realignment.  While the coherence with PMC HV may be gone, it might just be that the PMC HV signal is now burried in the noise of the ADC.  At a lockloss I went to the floor and measured HV mon, then plugged it into one of the 560s, AC coupled, 10 Hz high pass, gain of 100, and sent the output into H1:LSC-EXTRA_AI_1.  We still have high coherence with this channel and DARM.  (last attchment)

Also, the PMC realingment this morning did decrease the reflected power, but the transmitted power also dropped.

  refl(W) trans(W) sum(W) laser power out
July 20 126W 157 174
Yesterday 35 103 138 169
today 27 100 126 169

About turning the HPO on not adding noise:

Kiwamu pointed out that the uncalibrated comparison above showing that the noise did not get worse when the HPO came on was not as convincing as it should have been.  This morning he and I used the pcal line hieght to scale these uncalibrated spectra to something that should be proportional to meters, although we did not worry about frequency dependent calibration.  (4th screenshot)  From this you can see that the noise in July was very close to what it was in March before the HPO came on, but there is some stuff in the bucket that is a little worse.  

The point is made best by the last attached screenshot, which is nearly identical noise in the last good lock I could find before the HPO came on to the first decent lock after it came on. Pcal was not working at this time, so we can't use that to verify the calibration, but the input powers were similar (20Watts and 24 Watts), DCPD powers are both 20mA, and the DCPD whitening was on in both cases.  (The decimation filters were changed around the same time that the HPO came on which accounts for the difference at high frequencies.)

Images attached to this comment
jason.oberling@LIGO.ORG - 15:59, Thursday 20 October 2016 (30693)PSL

Regarding power available to the PMC, I know this is obvious but another thing we have to consider is the ISS.  Since the ISS AOM is before the PMC, it clearly also effects the amount of power available to the PMC.  Peter K. can correct me if I am wrong, but it is my understanding that this happens primarily in 2 ways:

  • Obviously if the ISS AOM is diffracting more light, the total amount of power availabe to the PMC decreases.
  • Related to the above, the ISS AOM can cause slight distortions in the beam profile, which is dependant on how hard the AOM is driven; the harder the AOM is driven, the more it distorts the beam.  These distortions cause changes to the mode matching into the PMC and therefore lower the visibility of the cavity.  This has the effect of increasing the reflected power and lowering the transmitted power.

On 2016-9-21, for reasons unknown to me, the ISS control offset was changed from ~4.3 to 20.  This means we are driving the ISS AOM much harder than we were previously.  This then causes changes in the beam profile, which effects the PMC mode matching and lowers the cavity visibility.  This is likely why, even though we have had only a 5W decrease in laser power since July, the total power into and the power transmitted by the PMC are down and the power reflected by the PMC has increased, and why we cannot return to the July PMC powers Sheila listed in her table in the above comment by simply tweaking the beam alignment into the PMC.  I have attached a 120 day minute-trend of the ISS control offset (H1:PSL-ISS_CTRL_OFFSET) that shows the changes in the ISS control offset value since 2016-6-22, including the 2016-9-21 change.  There are of course other reasons why the control offset changed (as can be seen on the attachment, the offset was changed several times over the last 4 months), the one on 9-21 just really stuck out.

Is there a reason why the control offset was changed so drastically?  Something to do with the new ISS outer loop electronics?

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