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ID Date Author Type Category Subject
  13110   Mon Jul 10 22:07:35 2017 KojiUpdateGeneralAll FEs down

I think this is the boot disk failure. I put the spare 2.5 inch disk into the slot #1. The OK indicator of the disk became solid green almost immediately, and it was recognized on the BIOS in the boot section as "Hard Disk". On the contrary, the original disk in the slot #0 has the "OK" indicator kept flashing and the BIOS can't find the harddisk.

 

  13109   Mon Jul 10 21:31:15 2017 KaustubhHowToComputer Scripts / ProgramsDetails on Cavity Scan Analysis

Summary:

The following elog describes the procedure followed for generating a sample simulation for a cavity scan, fitting an actual cavity scan and calculating the relevant paramaters using the cavity scan and fit data.

 

1. Cavity Scan Simulation:

  1. First, we define the sample cavity parameters, i.e., the reflectivitie,transmissivities of the mirrors, the RoCs of the mirrors and the absolute cavity length.
  2. We then define a frequency range using numpy.linspace function for which we want to take a scan.
  3. We then define a function that returns the tranmission power output of a Fabry-Perot cavity using the cavity equations as follows: P_{t} = \frac{t_{1}t_{2}}{1-r_{1}r_{2}\exp({\frac{4\pi Lf}{c}+(n+m+1)\phi_G)}} where Pt is the transmission power ratio of the output power to input power, t1,t2,r1,r2 are the transmissivities and reflectivities of the two mirrors, L is the absolute cavity length, f is the frequency of the input laser, c is the speed of light, \phi_G = \arccos{g_{1}g_{2}} is the gouy phase shift with g1,g2 being the g-factors for the two cavity mirrors(g=1-L/R). 'n' and 'm' correspond to the TEMnm higher order mode.
  4. We now obtain a cavity scan by giving the above defined function the cavity parameters and by adding the outputs for different higher order mode('n', 'm' values). Appropriate factors for the HOMs need to be chosen. The above function with appropriate coefficients can be used ti also add the modulated sidebands to the total transmission power.
  5. To this obtained total power we can add some random noise using numpy modules random.normal function. We need to normalise the data with respect to the max. power transmission ratio.
  6. We can now perform fitting on the above data using the procedure stated in the next section and then plot the two data sets using matplotlib module.
  7. A similar code to do the above is given here.

 

2. Fitting a Cavity Scan:

  1. The actual data for a cavity scan can be found in this elog entry or attached below in the zip folder.
  2. We read this data and separate the frequency data and the transmission data.
  3. Using the peakutils module's indexes function, we find the indices of the various peaks in the data set.
  4. These peaks are from the fundamental resonances, sideband resonances(both 11MHz and 55MHz) as well as a few HOMs.
  5. Each of these resonances follows the cavity equations and hence can be modelled as Lorentzian within small intervals around the peak frequencies. A detailed description of how this is possible is given here and is in the atached zip folder('Functionsused.pdf').
  6. We define a Lorentzian function which returns the fo\frac{a}{1+(\frac{\nu - \nu_0}{b})^{2}}llows:  where 'a' is the peak transmission value, 'b' is the 'linewidth' of the Lorentzian and \nu_0 is the peak frequency  about which the cavity equations behave like a lorentzian.
  7. We now, using the Lorentzian function, fit the various identified peaks using the curve_fit function of the scipy module. Remember to turn the 'absolute_sigma' parameter to 'True'.
  8. The parameters now obtained can be evaluated using the procedure given in the next section.
  9. The total transmission power is evaluated by feeding in the above obtained parameters back into the Lorentzian function and adding it for each peak.
  10. We can plot the actual data set and the data obtained using the fit of different peaks in a plot using matplotlib module. We can also plot the residuals for a better depiction of the fit quality.  
  11. The code to analyse the above mentioned cavity scan data is given here and attached below in the zip folder.

 

3. Calculating Physically Relevant Parameters:

  1. The data obtained from the fitting the peaks in the previous section now needs to be analysed in order to obtain some physically relevant information such as the FSR value, the TMS value, the modulation depths of the sidebands and perhaps even the linear caliberation of the frequency.
  2. First we need to identify the fundamental, TEM00 resonances among all the peaks. This we do by using the numpy.where function. We find the peaks with transmission values more than 0.9(or any suitable value).
  3. Using these indices we will now calculate the FSR and the Finesse of the peaks. A description of the correlation between the Fit Parameters and the FSR and Finesse is given here.
  4. We define a Linear fitting function for fitting the frequency values of the fundamental resonances against the ith fundamental resonance. The slope of this line gives us the value of FSR and the error in it.
  5. The Finesse can be calculated by fitting the linewidth with a constant function.
  6. The cavity length can be calculated using the FSR values as follows: L = \frac{c}{2\nu_{FSR}}.
  7. Now, the approximate positions of the sideband frequncies is given by 11*106%FSR and 55*106%FSR away from the fundamental, carrier resonances.
  8. The modulation depth, 'm', is given as \sqrt{\frac{P_{c}}{P_{s}}} = \frac{J_{0}(m)}{J_{1}(m)} where Pc is the carrier transmission power, Ps is the transmission power of the sideband and Jv is the Bessel Function of order 'v'.
  9. We define a function 'Bessel Ratio' using which we'll fit the transmission power ratio of the carrier to the sideband for the multiple sideband resonances.
  10. We also check for the Linearity in frequency data by plotting Fitting the frequencies corresponding to peaks in the actual data to ones obtained after fitting.
  11. After this we attempt to identify the other HOMs. For this we first determine a rough estimate for the value of TMS using the already known parameters of the mirrors,i.e., the RoC. We then look in small intervals (0.5 MHz) around frequencies where we would expect the HOMs to be, i.e., 1*TMS, 2*TMS, 3*TMS... away from the fundamental resonances. These positions are all modulo FSR.
  12. After identifying the HOMs, we take the difference from the fundamental resonance and then study these modulo the FSR.
  13. We perform a Linear Fit between these obtained values and (n+m).  As 'n','m' are degenerate, we can simply perform the fit against some variable 'k' and obtain the value of TMS as the slope of the linear fit.
  14. The code to do the above stated analysis is given here.

 

Most of the above info and some smaller details can be found in the markdown readme file in this git repo.

Attachment 1: Attachments.zip
  13108   Mon Jul 10 21:03:48 2017 jamieUpdateGeneralAll FEs down

 

Quote:
 

However, FB still will not boot up. The error is identical to that discussed in this thread by Intel. It seems FB is having trouble finding its boot disk. I was under the impression that only the FE machines were diskless, and that FB had its own local boot disk - in which case I don't know why this error is showing up. According to the linked thread, it could also be a problem with the network card/cable, but I saw both lights on the network switch port FB is connected to turn green when I powered the machine on, so this seems unlikely. I tried following the steps listed in the linked thread but got nowhere, and I don't know enough about how FB is supposed to boot up, so I am leaving things in this state now. 

It's possible the fb bios got into a weird state.  fb definitely has it's own local boot disk (*not* diskless boot).  Try to get to the BIOS during boot and make sure it's pointing to it's local disk to boot from.

If that's not the problem, then it's also possible that fb's boot disk got fried in the power glitch.  That would suck, since we'd have to rebuild the disk.  If it does seem to be a problem with the boot disk then we can do some invasive poking to see if we can figure out what's up with the disk before rebuilding.

  13107   Mon Jul 10 19:15:21 2017 gautamUpdateGeneralAll FEs down

The Jetstor RAID array is back in its nominal state now, according to the web diagnostics page. I did the following:

  1. Powered down the FB machine - to avoid messing around with the RAID array while the disks are potentially mounted.
  2. Turned off all power switches on the back of the Jetstor unit - there were 4 of them, all of them were toggled to the "0" position.
  3. Disconnected all power cords from the back of the Jetstor unit - there were 3 of them.
  4. Reconnected the power cords, turned the power switches back on to their "1" position.

After a couple of minutes, the front LCD display seemed to indicate that it had finished running some internal checks. The messages indicating failure of power units, which was previously constantly displayed on the front LCD panel, was no longer seen. Going back to the control room and checking the web diagnostics page, everything seemed back to normal.

However, FB still will not boot up. The error is identical to that discussed in this thread by Intel. It seems FB is having trouble finding its boot disk. I was under the impression that only the FE machines were diskless, and that FB had its own local boot disk - in which case I don't know why this error is showing up. According to the linked thread, it could also be a problem with the network card/cable, but I saw both lights on the network switch port FB is connected to turn green when I powered the machine on, so this seems unlikely. I tried following the steps listed in the linked thread but got nowhere, and I don't know enough about how FB is supposed to boot up, so I am leaving things in this state now. 

  13106   Mon Jul 10 17:46:26 2017 gautamUpdateGeneralAll FEs down

A bit more digging on the diagnostics page of the RAID array reveals that the two power supplies actually failed on Jun 2 2017 at 10:21:00. Not surprisingly, this was the date and approximate time of the last major power glitch we experienced. Apart from this, the only other error listed on the diagnostics page is "Reading Error" on "IDE CHANNEL 2", but these errors precede the power supply failure.

Perhaps the power supplies are not really damaged, and its just in some funky state since the power glitch. After discussing with Jamie, I think it should be safe to power cycle the Jetstor RAID array once the FB machine has been powered down. Perhaps this will bring back one/both of the faulty power supplies. If not, we may have to get new ones. 

The problem with FB may or may not be related to the state of the Jestor RAID array. It is unclear to me at what point during the boot process we are getting stuck at. It may be that because the RAID disk is in some funky state, the boot process is getting disrupted.

Quote:

I am unable to get FB to reboot to a working state. A hard reboot throws it into a loop of "Media Test Failure. Check Cable".

Jetstor RAID array is complaining about some power issues, the LCD display on the front reads "H/W Monitor", with the lower line cycling through "Power#1 Failed", "Power#2 Failed", and "UPS error". Going to 192.168.113.119 on a martian machine browser and looking at the "Hardware information" confirms that System Power #1 and #2 are "Failed", and that the UPS status is "AC power loss". So far I've been unable to find anything on the elog about how to handle this problem, I'll keep looking.


In fact, looks like this sort of problem has happened in the past. It seems one power supply failed back then, but now somehow two are down (but there is a third which is why the unit functions at all). The linked elog thread strongly advises against any sort of power cycling. 

 

  13105   Mon Jul 10 17:13:21 2017 jigyasaUpdateComputer Scripts / ProgramsCapture image without pylon GUI

Over the day, I have been working on a C++ program to interface with Pylon to capture images and reduce dependence on the Pylon GUI. The program uses the Pylon header files along with opencv headers. While ultimately a wrapper in python may be developed for the program, the current C++ program at, 

/users/jigyasa/GigEcode/Grab/Grab.cpp when compiled as

g++ -Wl,--enable-new-dtags -Wl,-rpath,/opt/pylon5/lib64 -o Grab Grab.o -L/opt/pylon5/lib64 -Wl,-E -lpylonbase -lpylonutility -lGenApi_gcc_v3_0_Basler_pylon_v5_0 -lGCBase_gcc_v3_0_Basler_pylon_v5_0 `pkg-config opencv --cflags --libs`

returns an executable file named Grab which can be executed as ./Grab

This captures one image from the camera and displays it, additionally it also displays the gray value of the first pixel.

I am working on adding more utility to the program such as manually adjusting exposure, gain and also on the python wrapper (Cython has been installed locally on Ottavia for the purpose)!

  13104   Mon Jul 10 11:20:20 2017 gautamUpdateGeneralAll FEs down

I am unable to get FB to reboot to a working state. A hard reboot throws it into a loop of "Media Test Failure. Check Cable".

Jetstor RAID array is complaining about some power issues, the LCD display on the front reads "H/W Monitor", with the lower line cycling through "Power#1 Failed", "Power#2 Failed", and "UPS error". Going to 192.168.113.119 on a martian machine browser and looking at the "Hardware information" confirms that System Power #1 and #2 are "Failed", and that the UPS status is "AC power loss". So far I've been unable to find anything on the elog about how to handle this problem, I'll keep looking.


In fact, looks like this sort of problem has happened in the past. It seems one power supply failed back then, but now somehow two are down (but there is a third which is why the unit functions at all). The linked elog thread strongly advises against any sort of power cycling. 

  13103   Mon Jul 10 09:49:02 2017 gautamUpdateGeneralAll FEs down

Attachment #1: State of CDS overview screen as of 9.30AM today morning when I came in.

Looks like there may have bene a power glitch, although judging by the wall StripTool traces, if there was one, it happened more than 8 hours ago. FB is down atm so can't trend to find out when this happened.

All FEs and FB are unreachable from the control room workstations, but Megatron, Optimus and Chiara are all ssh-able. The latter reports an uptime of 704 days, so all seems okay with its UPS. Slow machines are all responding to ping as well as telnet.

Recovery process to begin now. Hopefully it isn't as complicated as the most recent effort indecision[FAMOUS LAST WORDS]

Attachment 1: CDS_down_10Jul2017.png
CDS_down_10Jul2017.png
  13102   Sun Jul 9 08:58:07 2017 ranaUpdateGeneralETMY TRANS QPD anomaly

Indeed, the whole point of the high/low gain setup is to never use the QPDs for the single arm work. Only use the high gain Thorlabs PD and then the switchover code uses the QPD once the arm powers are >5.

I don't know how the operation procedure went so higgledy piggledy.

  13101   Sat Jul 8 17:09:50 2017 gautamUpdateGeneralETMY TRANS QPD anomaly

About 2 weeks ago, I noticed some odd behaviour of the LSC TRY data stream. Its DC value seems to be drifting ~10x more than TRX. Both signals come from the transmission QPDs. At the time, we were dealing with various CDS FE issues but things have been stable on that end for the last two weeks, so I looked into this a bit more today. It seems like one particular channel is bad - Quadrant 4 of the ETMY TRANS QPD. Furthermore, there is a bump around 150Hz, and some features above 2kHz, that are only present for the ETMY channels and not the ETMX ones.

Since these spectra were taken with the PSL shutter closed and all the lab room lights off, it would suggest something is wrong in the electronics - to be investigated.

The drift in TRY can be as large as 0.3 (with 1.0 being the transmitted power in the single arm lock). This seems unusually large, indeed we trigger the arm LSC loops when TRY > 0.3. Attachment #2 shows the second trend of the TRX and TRY 16Hz EPICS channels for 1 day. In the last 12 hours or so, I had left the LSC master switch OFF, but the large drift of the DC value of TRY is clearly visible.

In the short term, we can use the high-gain THORLABS PD for TRY monitoring.

Attachment 1: ETMY_QPD.pdf
ETMY_QPD.pdf
Attachment 2: ETMY_QPD.png
ETMY_QPD.png
  13100   Fri Jul 7 14:34:27 2017 ranaUpdateCamerasHDR images of ETMX

i wonder how 'HDR' these images really are. is there a quantitative way to check that we are really getting more bits? also, how many bits does the PNG format allow for monochrome images? i worry that these elog images are already lossy.

 

  13099   Fri Jul 7 09:03:40 2017 SteveSummaryHistoryas it was in 1994


 

Attachment 1: 1994.PDF
1994.PDF 1994.PDF
  13098   Thu Jul 6 11:58:28 2017 jigyasaUpdateCamerasHDR images of ETMX

I captured a few images of the beam spot on ETMX at 5ms, 10ms, 14ms, 50ms, 100ms, 500ms, 1000ms exposure and ran them through my python script for HDR images. Here's what I obtained. 
The resulting image is an improvement over the highly saturated images at say, 500ms and 1 second exposures. 
Additionally, I also included a colormapped version of the image. 

Attachment 1: ETMXHDRcolormap.png
ETMXHDRcolormap.png
Attachment 2: ETMXHDRimage.png
ETMXHDRimage.png
  13097   Wed Jul 5 19:10:36 2017 gautamUpdateGeneralNB code checkout - updated

I've been making NBs on my laptop, thought I would get the copy under version control up-to-date since I've been negligent in doing so.

The code resides in /ligo/svncommon/NoiseBudget, which as a whole is a git directory. For neatness, most of Evan's original code has been put into the sub-directory  /ligo/svncommon/NoiseBudget/H1NB/, while my 40m NB specific adaptations of them are in the sub-directory /ligo/svncommon/NoiseBudget/NB40. So to make a 40m noise budget, you would have to clone and edit the parameter file accordingly, and run python C1NB.py C1NB_2017_04_30.py for example. I've tested that it works in its current form. I had to install a font package in order to make the code run (with sudo apt-get install tex-gyre ), and also had to comment out calls to GwPy (it kept throwing up an error related to the package "lal", I opted against trying to debug this problem as I am using nds2 instead of GwPy to get the time series data anyways).

There are a few things I'd like to implement in the NB like sub-budgets, I will make a tagged commit once it is in a slightly neater state. But the existing infrastructure should allow making of NBs from the control room workstations now.

Quote:

[evan, gautam]

We spent some time trying to get the noise-budgeting code running today. I guess eventually we want this to be usable on the workstations so we cloned the git repo into /ligo/svncommon. The main objective was to see if we had all the dependencies for getting this code running already installed. The way Evan has set the code up is with a bunch of dictionaries for each of the noise curves we are interested in - so we just commented out everything that required real IFO data. We also commented out all the gwpy stuff, since (if I remember right) we want to be using nds2 to get the data. 

Running the code with just the gwinc curves produces the plots it is supposed to, so it looks like we have all the dependencies required. It now remains to integrate actual IFO data, I will try and set up the infrastructure for this using the archived frame data from the 2016 DRFPMI locks..

 

  13096   Wed Jul 5 16:09:34 2017 gautamUpdateCDSslow machine bootfest

Reboots for c1susaux, c1iscaux today.

 

  13095   Wed Jul 5 10:23:18 2017 SteveUpdatesafetyliquid nitrogen boil off

The liquid nitrogen container has a pressure releif valve set to 35 PSI  This valve will open periodically when contains LN2

The exiting  very cold gas can cause burning so it should not hit directly your eyes or skin.  Set the pointing of this valve into the corner.

Leave entry door open so nitrogen concentration can not build up.

Oxygen deficiency
Nitrogen can displace oxygen in the air, reducing the
percentage of oxygen to below safe levels. Because the brain
needs a continuous supply of oxygen to remain active, lack
of oxygen prevents the brain from functioning properly, and
it shuts down.
Being odorless, colorless, tasteless, and nonirritating,
nitrogen has no properties that can warn people of its pres-
ence. Inhalation of excessive amounts of nitrogen can cause
dizziness, nausea, vomiting, loss of consciousness, and death
Attachment 1: liqued_nitrogen_boil_off.jpg
liqued_nitrogen_boil_off.jpg
  13094   Sat Jul 1 14:27:00 2017 KojiUpdateGeneralDRMI re-locked

Basically we use the arm cavities as the reference of the beam alignment. The incident beam is aligned such that the ITMY angle dither is minimized (at least at the dither freq).
This means that we have no capability to adjust the spot poisitions on the PRM, SRM, BS, ITMX optics.

We are still able to minimize A2L by adding intentional asymmetry to the coil actuators.

  13093   Fri Jun 30 22:28:27 2017 gautamUpdateGeneralDRMI re-locked

Summary:

Reverted to old settings, tried to reproduce DRMI lock with settings as close to those used in May this year as possible. Tonight, I was successful in getting a couple of ~10min DRMI 1f locks yes. Now I can go ahead and try and reduce the noise.

I am not attempting a full characterization tonight, but the important changes since the May locks are in the de-whitening boards and coil driver boards. I did not attempt to engage the coil-dewhitening, but the PD whitening works fine.

As a quick check, I tested the hypothesis that the BS OL loop A2L coupling dominates between ~10-50Hz. The attached control signal spectra [Attachment #2] supports this hypothesis. Now to actually change the loop shape.

I've centered Oplevs of all vertex optics, and also the beams on the REFL and AS PDs. The ITMs and BS have been repeatedly aligned since re-installing their respective coil driver electronics, but the SRM alignment needed some adjustment of the bias sliders.

Full characterization to follow. Some things to check:

  • Investigate adn fix the suspect X-arm ASS loop
  • Is there too much power on the AS110 PD post Oct2016 vent? Is the PD saturating?

Lesson learnt: Don't try and change too many things at once!

GV July 5 1130am: Looks like the MICH loop gain wasn't set correctly when I took the attached spectra, seems like the bump around 300Hz was caused by this. On later locks, this feature wasn't present.

Attachment 1: DRMI_relocked.png
DRMI_relocked.png
Attachment 2: MICH_OL.pdf
MICH_OL.pdf
  13092   Fri Jun 30 16:03:54 2017 jigyasaUpdateCamerasGigE camera at ETMX

 

Quote:

All thanks to Steve, we cleaned the view port on the ETMX on which the camera is installed, and with a little fine tuning of the focus of the camera, here's a really good image of the beam spot at 6 and 14 ms.

Quote:
Steve's note: AR coated camera lens M5018-SW installed at ~40 degrees

 

 

Attachment 1: 14msexposure.png
14msexposure.png
  13091   Fri Jun 30 15:25:19 2017 jigyasaUpdateCamerasGigE camera at ETMX

All thanks to Steve, we cleaned the view port on the ETMX on which the camera is installed, and with a little fine tuning of the focus of the camera, here's a really good image of the beam spot at 6 and 14 ms.

Quote:
Steve's note: AR coated camera lens M5018-SW installed at ~40 degrees

 

Attachment 1: Image__2017-06-30__15-10-05.pdf
Image__2017-06-30__15-10-05.pdf
Attachment 2: 14ms.pdf
14ms.pdf
  13090   Fri Jun 30 11:50:17 2017 gautamUpdateGeneralDRMI locking attempt

Seems like the problem is actually with ITMX - the attached DV plots are for ITMX with just local damping loops on (no OLs), LR seems to be suspect.

I'm going to go squish cables and the usual sat. box voodoo, hopefully that settles it.

Quote:

Summary:

I attempted to re-lock the DRMI and try and realize some of the noise improvements we have identified. Summary elog, details to follow.

  1. Locked arms, ran ASS, centered OLs on ITMs and BS on their respective QPDs.
  2. Looked into changing the BS Oplev loop shape to match that of the ITMs - it looks like the analog electronics that take the QPD signals in for the BS Oplev is a little different, the 800Hz poles are absent. But I thought I had managed to do this successfully in that the error signal suppression improved and it didn't look like the performance of the modified loop was worse anywhere except possibly at the stack resonance of ~3Hz --- see Attachment #1 (will be rotated later). The TRX spectra before and after this modification also didn't raise any red flags.
  3. Re-aligned PRM - went to the AS table and centered beam on all REFL PDs
  4. Locked PRMI on carrier, ran MICH and AS dither alignment. PRC angular feedforward also seemed to work well.
  5. Re-aligned SRM, looked for DRMI locks - there was a brief lock of a couple of seconds, but after this, the BS behaviour changed dramatically.

Basically after this point, I was unable to repeat stuff I did earlier in the evening just a couple of hours ago. The single arm locks catch quickly, and seem stable over the hour timescale, but when I run the X arm dither, the BS PITCH loop starts to oscillate at ~0.1 Hz. Moreover, I am unable to acquire PRMI carrier lock. I must have changed a setting somewhere that I am not catching right now (although I've scripted most of these things for repeatability, so I am at a loss what I'm missing indecision). The only change I can think of is that I changed the BS Oplev loop shape. But I went back into the filter file archives and restored these to their original configuration. Hopefully I'll have better luck figuring this out tomorrow.

 

Attachment 1: ITMX_glitchy.png
ITMX_glitchy.png
  13089   Fri Jun 30 11:08:26 2017 jigyasaUpdateCamerasGigE camera at ETMX
With Steve's help in getting the right depth of field for imaging and focusing on the test mass with the new AR coated lens, Gautam's help with locking the arm and trying my hand at adjusting the focus of the camera yesterday, we were able to get some images of the IR beam, with the green shutter on and off at different exposures. Since the CCD is at an angle to the optic, the exposure time had to be increased signifcantly(and varied between 0.08 to 0.5 seconds) to capture bright images. 
A few frames without the IR on and with the green shutter closed were captured.
These show the OSEM and the Oplev on the test mass. 
 
Steve's note: AR coated camera lens M5018-SW installed at ~40 degrees
                    Atm2,  pcicture is taken through dirty window
 
Quote:

Also the GigE has been wired and conencted to the Martian. Image acquisition is possible with Pylon.

 

 

Attachment 1: PicturesETMX.pdf
PicturesETMX.pdf PicturesETMX.pdf PicturesETMX.pdf PicturesETMX.pdf
Attachment 2: dirtyETMXwindow.jpg
dirtyETMXwindow.jpg
  13088   Fri Jun 30 02:13:23 2017 gautamUpdateGeneralDRMI locking attempt

Summary:

I attempted to re-lock the DRMI and try and realize some of the noise improvements we have identified. Summary elog, details to follow.

  1. Locked arms, ran ASS, centered OLs on ITMs and BS on their respective QPDs.
  2. Looked into changing the BS Oplev loop shape to match that of the ITMs - it looks like the analog electronics that take the QPD signals in for the BS Oplev is a little different, the 800Hz poles are absent. But I thought I had managed to do this successfully in that the error signal suppression improved and it didn't look like the performance of the modified loop was worse anywhere except possibly at the stack resonance of ~3Hz --- see Attachment #1 (will be rotated later). The TRX spectra before and after this modification also didn't raise any red flags.
  3. Re-aligned PRM - went to the AS table and centered beam on all REFL PDs
  4. Locked PRMI on carrier, ran MICH and AS dither alignment. PRC angular feedforward also seemed to work well.
  5. Re-aligned SRM, looked for DRMI locks - there was a brief lock of a couple of seconds, but after this, the BS behaviour changed dramatically.

Basically after this point, I was unable to repeat stuff I did earlier in the evening just a couple of hours ago. The single arm locks catch quickly, and seem stable over the hour timescale, but when I run the X arm dither, the BS PITCH loop starts to oscillate at ~0.1 Hz. Moreover, I am unable to acquire PRMI carrier lock. I must have changed a setting somewhere that I am not catching right now (although I've scripted most of these things for repeatability, so I am at a loss what I'm missing indecision). The only change I can think of is that I changed the BS Oplev loop shape. But I went back into the filter file archives and restored these to their original configuration. Hopefully I'll have better luck figuring this out tomorrow.

Attachment 1: BS_OLmods.pdf
BS_OLmods.pdf
  13087   Thu Jun 29 10:04:18 2017 jigyasaUpdateComputer Scripts / ProgramsMC2 Pitch-Yaw offset

The script is being executed again, now.

Quote:

I worked on the code today and have left a script (MC2rerun.py) running on Ottavia which should run overnight.

 

 

  13086   Thu Jun 29 00:13:08 2017 KaustubhUpdateComputer Scripts / ProgramsTransfer Function Testing

In continuation to my previous posts, I have been working on evaluating the data on transfer function. Recently, I have calculated the correlation values between the real and imaginary part of the transfer function. Also I have written the code for plotting the transfer function data stream at each frequency in the argand plane just for referring to. Also I have done a few calculations and found the errors in magnitude and phase using those in the real and imaginary parts of the transfer function. More details for the process are in this git repository.

The following attachments have been added:

  1. The correlation plot at different frequencies. This data is for a 100 data files.
  2. The Test files used to produce the abover plot along with the code for the plotting it as well as the text file containing the correlation values. (Most of the code is commented as that part wasn't needed fo rhte recent changes.)

 

Conclusion:

Seeing the correlation values, it sounds reasonable that the gaussian in real and imaginary parts approximation is actually holding. This is because the correlation values are mostly quite small. This can be seen by studying the distribution of the transfer function on the argand plane. The entire distribution can be seen to be somewhat, if not entirely, circular. Even when the ellipticity of the curve seems to be high, the curve still appears to be elliptical along the real and imaginary axes, i.e., correlation in them is still low.

 

To Do:

  1. Use a better way to estimate the errors in magnitude and phase as the method used right now is a only valid with the liner approximation and gives insane values which are totally out of bounds when the magnitude is extrmely small and the phase is varying as mad.
  2. Use the errors in the transfer function to estimate the coherence in the data for each frequency point. That is basically plot a cohernece Vs frequency plot showing how the coherence of the measurements vary as the frequency is varied.

 

In order to test the above again, with an even larger data set, I am leaving a script running on Ottavia. It should take more than just the night(I estimate around 10-11 hours) if there are no problems.

Attachment 1: Correlation_Plot.pdf
Correlation_Plot.pdf
Attachment 2: 2x100_Test_Files_and_Code_and_Correlation_Files.zip
  13085   Wed Jun 28 20:15:46 2017 gautamUpdateGeneralc1iscex timing troubles

[Koji, gautam]

Here is a summary of what we did today to fix the timing issue on c1iscex. The power supply to the timing card in the X end expansion chassis was to blame.

  1. We prepared the Y-end expansion chassis for transport to the X end. To do so, we disconnected the following from the expansion chassis
    • Cables going to the ADC/DAC adaptor boards
    • Dolphin connector
    • BIO connector
    • RFM fiber
    • Timing fiber
  2. We then carried the expansion chassis to the X end electronics rack. There we repeated the above steps for the X-end expansion chassis
  3. We swapped the X and Y end expansion chassis in the X end electronics rack. Powering the unit, we immediately saw the green lights on the front of the timing card turn on, suggesting that the Y-end expansion chassis works fine at the X end as well (as it should). To further confirm that all was well, we were able to successfully start all the RT models on c1iscex without running into any timing issues.
  4. Next, we decided to verify if the spare timing card is functional. So we swapped out the timing card in the expansion chassis brought over to the X end from the Y end with the spare. In this test too, all worked as expected. So at this stage, we concluded that
    • There was nothing wrong with the fiber bringing the timing signal to the X end
    • The Y-end expansion chassis works fine
    • The spare timing card works fine.
  5. Then we decided to try the original X-end expansion chassis timing card in the Y-end expansion chassis. This test too was successful - so there was nothing wrong with any of the timing card!
  6. Next, we decided to power the X-end timing chassis with its original timing card, which was just verified to work fine. Surprisingly, the indicator lights on the timing card did not turn on.
  7. The timing card has 3 external connections
    • A 40 pin IDE connector
    • Power
    • Fiber carrying the timing signal
  8. We went back to the Y-end expansion chassis, and checked that the indicator lights on the timing card turned on even when the 40 pin IDE connector was left unconnected (so the timing card just gets power and the timing signal).
  9. We concluded that the power supply in the X end expansion chassis was to blame. Indeed, when Koji jiggled the connector around a little, the indicator lights came on!
  10. The connection was diagnosed to be somewhat flaky - it employs the screw-in variety of terminal blocks, and one of the connections was quite loose - Koji was able to pull the cable out of the slot applying a little pressure.
  11. I replaced the cabling (swapped the wires for thicker gauge, more flexible variety), and re-tightened the terminal block screws. The connection was reasonably secure even when I applied some force. A quick test verified that the timing card was functional when the unit was powered.
  12. We then replaced the X and Y-end expansion chassis (complete with their original timing cards, so the spare is back in the CDS cabinet), in the racks. The models started up again without complaint, and the CDS overview screen is now in a good state [Attachment #1]. The arms are locked and aligned for maximum transmission now.
  13. There was some additional difficulty in getting the 40-pin IDE connector in on the Y-end expansion chassis. Looked like we had bent some of the pins on the timing board while pulling this cable out. But Koji was able to fix this with a screw driver. Care should be taken when disconnecting this cable in the future!

There were a few more flaky things in the Expansion chassis - the IDE connectors don't have "keys" that fix the orientation they should go in, and the whole timing card assembly is kind of difficult and not exactly secure. But for now, things are back to normal it seems.

Wouldn't it be nice if this fix also eliminates the mystery ETMX glitching problem? After all, seems like this flaky power supply has been a problem for a number of years. Let's keep an eye out.

Attachment 1: CDS_status_28Jun2017.png
CDS_status_28Jun2017.png
  13084   Tue Jun 27 18:47:49 2017 jigyasaUpdateComputer Scripts / ProgramsMC2 Pitch-Yaw offset

The values generated from the script were analyzed and a 3D scatter plot in addition to a 2D map were plotted. 

Yesterday, Rana pointed me to another method of collecting and analyzing the data. So I worked on the code today and have left a script (MC2rerun.py) running on Ottavia which should run overnight.

Quote:

The script didn't run properly last night, due to an oversight of variable names! It's been started again and has been running for half an hour now.

 

 

  13083   Tue Jun 27 16:18:59 2017 jigyasaUpdateCamerasGigE camera at ETMX

The 50mm lens has arrived. (Delivered yesterday).

Also the GigE has been wired and conencted to the Martian. Image acquisition is possible with Pylon.

Quote:

GigE can be connected to ethernet. AR coated 1064 f50 can arrive any day now.

 

  13082   Tue Jun 27 16:11:28 2017 gautamUpdateElectronicsCoil whitening

I got back to trying to engage the coil driver whitening today, the idea being to try and lock the DRMI in a lower noise configuration - from the last time we had the DRMI locked, it was determined that A2L coupling from the OL loops and coil driver noise were dominant from ~10-200Hz. All of this work was done on the Y-arm, while the X-arm CDS situation is being resolved.

To re-cap, every time I tried to do this in the last month or so, the optic would get kicked around. I suspected that the main cause was the insufficient low-pass filtering on the Oplev loops, which was causing the DAC rms to rail when the whitening was turned on. 

I had tried some loop-tweaking by hand of the OL loops without much success last week - today I had a little more success. The existing OL loops are comprised of the following:

  • Differentiator at low frequencies (zero at DC, 2 poles at 300Hz)
  • Resonant gain peaked around 0.6 Hz with a Q of ______ (to be filled in)
  • BR notches 
  • A 2nd order elliptic low pass with 2dB passband ripple and 20dB stopband attenutation

THe elliptic low pass was too shallow. For a first pass at loop shaping today, I checked if the resonant gain filter had any effect on the transmitted power RMS profile - turns out it had negligible effect. So I disabled this filter, replaced the elliptic low pass with a 5th order ELP with 2dB passband ripple and 80dB stopband attenuation. I also adjusted the overall loop gain to have an upper UGF for the OL loops around 2Hz. Looking at the spectrum of one coil output in this configuration (ITMY UL), I determined that the DAC rms was no longer in danger of railing.

However, I was still unable to smoothly engage the de-whitening. The optic again kept getting kicked around each time I tried. So I tried engaging the de-whitening on the ITM with just the local damping loop on, but with the arm locked. This transition was successful, but not smooth. Looking at the transmon spot on the camera, every time I engage the whitening, the spot gets a sizeable kick (I will post a video shortly).  In my ~10 trials this afternoon, the arm is able to stay locked when turning the whitening on, but always loses lock when turning the whitening off. 

The issue here is certainly not the DAC rms railing. I had a brief discussion with Gabriele just now about this, and he suggested checking for some electronic voltage offset between the two paths (de-whitening engaged and bypassed). I also wonder if this has something to do with some latency between the actual analog switching of paths (done by a slow machine) and the fast computation by the real time model? To be investigated.

GV 170628 11pm: I guess this isn't a viable explanation as the de-whitening switching is handled by the one of the BIO cards which is also handled by the fast FEs, so there isn't any question of latency.

With the Oplev loops disengaged, the initial kick given to the optic when engaging the whitening settles down in about a second. Once the ITM was stable again, I was able to turn on both Oplev loops without any problems. I did not investigate the new Oplev loop shape in detail, but compared to the original loop shape, there wasn't a significant difference in the TRY spectrum in this configuration (plot to follow). This remains to be done in a systematic manner. 

Plots to support all of this to follow later in the evening.

Attachment #1: Video of ETMY transmission CCD while engaging whitening. I confirmed that this "glitch" happens while engaging the whitening on the UL channel. This is reminiscent of the Satellite Box glitches seen recently. In that case, the problem was resolved by replacing the high-current buffer in the offending channel. Perhaps something similar is the problem here?

Attachment #2: Summary of the ITMY UL coil output spectra under various conditions.

 

Attachment 1: ETMYT_1182669422.mp4
Attachment 2: ITMY_whitening_studies.pdf
ITMY_whitening_studies.pdf
  13081   Mon Jun 26 22:01:08 2017 KojiUpdateGeneralc1iscex timing troubles

I tried a couple of things, but no fundamental improvement of the missing LED light on the timing board.

- The power supply cable to the timing board at c1iscex indicated +12.3V

- I swapped the timing fiber to the new one (orange) in the digital cabinet. It didn't help.

- I swapped the opto-electronic I/F for the timing fiber with the Y-end one. The X-end one worked at Y-end, and Y-end one didn't work at X-end.

- I suspected the timing board itself -> I brought a "spare" timing board from the digital cabinet and tried to swap the board. This didn't help.

 

Some ideas:

- Bring the X-end fiber to C1SUS or C1IOO to see if the fiber is OK or not.

- We checked the opto-electronic I/F is OK

- Try to swap the IO chassis with the Y-end one.

- If this helps, swap the timing board only to see this is the problem or not.

  13080   Mon Jun 26 09:39:15 2017 NaomiSummaryGeneralMeasure transfer functions of Mini-Circuits filters

I have spent my first few days as a SURF getting experience working with the Network/Spectrum Analyzer (AG 4395A). After an introduction to the 40m by Koji, I was tasked with using the AG4395A to measure the transfer function of several filters (for example, Mini-Circuits Low Pass Filter SLP-30). I am now familiar with configuring the AG 4395A, taking a single set of data using a command from one of the control computers, and plotting the dataset as a Bode plot (separate plots for magnitude and phase) using Python.

To Do:

  • Use AGmeasure to take multiple datasets with a single command.
  • Plot multiple datasets for each filter on a single Bode plot and perform some statistical analysis. 

To experiment with plotting multiple datasets on a single Bode plot, I used a single dataset from the Network Analyzer using the SLP-30 filter and added random noise to create ten datasets to plot. I am attaching the resulting Bode plot, which has the ten generated sets of data plotted along with their average.

We discussed with Rana and Koji how to interpret this type of dataset from the Network Analyzer. Instead of considering the magnitude and phase as separate quantities, we should consider them together as a single complex number in the form H(f) = M exp(iπP/180), where M is the magnitude and P is the phase in degrees. We can then find the average value of the measured quantity in its complex number form (x + iy), as opposed to just taking the average of the magnitude and phase separately.  

Attachment 1: Bode_Plot.png
Bode_Plot.png
  13079   Sun Jun 25 22:30:57 2017 gautamUpdateGeneralc1iscex timing troubles

I saw that the CDS overview screen indicated problems with c1iscex (also ETMX was erratic). I took a closer look and thought it might be a timing issue - a walk to the X-end confirmed this, the 1pps status light on the timing slave card was no longer blinking. 

I tried all versions of power cycling and debugging this problem known to me, including those suggested in this thread and from a more recent time. I am leaving things as it for the night, will look into this more tomorrow. I've also shutdown the ETMX watchdog for the time being. Looks like this has been down since 24Jun 8am UTC.

Attachment 1: c1iscex_status.png
c1iscex_status.png
  13078   Fri Jun 23 02:55:18 2017 KaustubhUpdateComputer Scripts / ProgramsScript Running

I am leaving a script running on the Pianoso for the night. For this purpose, even the AG4395A is kept on. I'll see the result of the script in the morning (it should be complete by then). Just check so before fiddling with the Analyzer.

Thank you.

  13077   Fri Jun 23 02:43:43 2017 KaustubhHowToComputer Scripts / ProgramsTaking Measurements From AG4395A

Summary:

I have written a code(a basic one which needs a lot of improvements, but still does the job) for taking multiple measurements from the AG4395A. I have also written a separate code for plotting the data taken from the previoius code along with the error bars upto 1 standard deviation.

 

Details on How To Operate AG4395A:

  1. Under 'Measurement' tab, press the 'Meas' button and select the Analyzer Type (Network Analyzer or Spectrum Analyzer).
  2. Then under the same options select which 'ratio' needs to be measured (A/R, B/R or A/B).
  3. Then press the 'Format' button to select what needs to be measured (Eg - Log|Mag|, Phase, etc.).
  4. In order to measure and see two channels at the same time (Eg - Log|Mag| and Phase), press the 'Display' button and select 'Dual Channel'.
  5. Using the 'Scale' button we can set the scale/div or use autoscale and also set the attenuator values of the different channels.
  6. The 'Bw/Avg' option gives us an averaging option which averages few sets of data to produce the result. In doing this we lose quiet a lot of data and the resulting plot isn't able to give us the information on the statistical errors.
  7. This option also allows us to set the 'Intermediate Frequency' Bandwidth. This basically dictates the sampling rate of the Analyzer. The lower the IF bw, the higher is lesser is the noise (due to less uncertainty in Frequency).
  8. The 'Cal' button helps us calibrate the Analyzer to the current connections and signals. This is done because there is usually a difference in the 'cable lengths' for the two channels which introduces an extra phase term depnding upon the rf frequency. The calibration can be simply done by removing the Device Under Test (DUT) and diectly connecting the coaxial cables to the channels. After this the 'Calibrate Menu' allows us to calibrate the response using the short, open and thru methods.
  9. Now, under the 'Sweep' tab, the 'Sweep' button allows us to select various sweep options such as 'Sweep Time' (Auto, or set a time), 'Number of Points' (b/w 201-801) and 'Sweep Type' (Linear, Log, List Freq. etc.).
  10. Using the 'Source' button we can set the source power in dBm units (Usually kept as -20 to -10 dBm).
  11. The Scan Range can be set in a few ways such as using the start and end points or using the center and span range/width.
  12. After setting up all of the above, we can take the measurement either from the analyzer itself or using one of the control PCs. The command to download the data from AG4395A is netgpibdata -i 192.168.113.105 -d AG4395A -a 10 -f [filename].

 

Brief Details on How the 'AGmeasure' command works:

AGmeasure is a python script developed by some of the people who work at 40m. It is set as a global command and can be used from within any directory. The source code is in the scripts folder on the network, or else it can also be found in Eric Quintero's git repository. This command accepts at the very least a parameter file. This is supposed to be a .yml file. A template (TFAG4395Atemplate.yml) can be found in the scripts folder or in Eric's repo. There are some other options that can be passed to this command, see the help for more details.

 

The Multi_Measurement Script:

This script calls the 'AGmeasure' command repetitively and keeps storing the data files in a folder. Right now, the script needs to be fed in th template file manually at prompt.

 

The Test_Plotting Script:

This script plots the a set of data files obtained from the above mentioned script and produces a plot along with the errors bands upto 1 standard deviation of the data. The format (names) and total number of text files need to be explicitly known, for now at least.

 

Attachments:

  1. The output test files and the two scripts.
  2. This is the 'Bode Plot' for a data set made using the above two scripts.

 

To Do:

  • Improve upon the two scripts to be as compatible as the AGmeasure function itself.
  • Try and incorporate the whole script into AGmeasure itself along with improving upon the templates.
  • The above details, with some edits perhaps, can go into the 40m wiki too(?).

 

Update: Increased the font size in the plot. Added a few comments to the two scripts

To Do: Need to consider the transfer function as a single physical quantity (both the magnitude and phase) and then take the averages and calculate the standard deviation and then plot these results. 

 

EDIT:

The attachment with the test files and the code now also contains a pdf with all the relations/equations I have used to calculate the averages and errors.

Attachment 1: Test_Files_and_Code.zip
Attachment 2: Bode_Plot_with_Error_Bands.pdf
Bode_Plot_with_Error_Bands.pdf
  13076   Tue Jun 20 17:44:12 2017 jigyasaUpdateComputer Scripts / ProgramsMC2 Pitch-Yaw offset

The script didn't run properly last night, due to an oversight of variable names! It's been started again and has been running for half an hour now.

Quote:

I am starting it on Donatella and it should run for a couple of hours.

Apologies for the inconvenience.

Quote:

A python script to randomly vary the MC2 pitch and yaw offset and correspondingly record the value of MC transmission has been started on Donatella in the control room and should run for a couple of hours overnight.

The script is named MC_TRANS_1.py and is located in my user directory at /users/jigyasa

 

  13075   Tue Jun 20 16:28:23 2017 SteveUpdateVACRGA scan
Attachment 1: RGAscan243d.png
RGAscan243d.png
Attachment 2: RGAscan.png
RGAscan.png
  13074   Tue Jun 20 14:58:08 2017 SteveUpdateCamerasGigE camera at ETMX

GigE can be connected to ethernet. AR coated 1064 f50 can arrive any day now.

Quote:

One of the additional GigE cameras has been IP configured for use and installation. 

Static IP assigned to the camera- 192.168.113.152
Subnet mask- 255.255.255.0
Gateway- 192.168.113.2
 

 

Attachment 1: ETMXgige.jpg
ETMXgige.jpg
  13073   Mon Jun 19 18:41:12 2017 jigyasaUpdateComputer Scripts / ProgramsMC2 Pitch-Yaw offset

The previous run of the script had produced some dubious results!

The script has been modified and now scans the transmission sum for a longer duration to provide a better estimate on the average transmission. The pitch and yaw offsets have been set to the values that were randomly generated in the previous run as this would enable comparison with the current data.

I am starting it on Donatella and it should run for a couple of hours.

Apologies for the inconvenience.

Quote:

A python script to randomly vary the MC2 pitch and yaw offset and correspondingly record the value of MC transmission has been started on Donatella in the control room and should run for a couple of hours overnight.

The script is named MC_TRANS_1.py and is located in my user directory at /users/jigyasa

  13072   Mon Jun 19 18:32:18 2017 jigyasaUpdateComputer Scripts / ProgramsSoftware Installation for image analysis

The IRAF software from the National Optical Astronomy Observatory has been installed locally on Donatella(for testing) following the instructions listed here at http://www.astronomy.ohio-state.edu/~khan/iraf/iraf_step_by_step_installation_64bit
This is a step towards "aperture photometry" and would help identify point scatterers in the images of the test masses.

I will be testing this software, in particular, the use of DAOPHOT and if it seems to work out, we may install it on the shared directory.
Hope this isn't an inconvenience.

 

 

  13071   Fri Jun 16 23:27:19 2017 Kaustubh, JigyasaUpdateComputersOttavia Connected to the Netgear Box

I just connected the Ottavia to the Netgear box and its working just fine. It'll remain switched on over the weekend.

Quote:

Kaustubh and I are going to enable the ethernet connection to Ottavia and secure the wiring now.  

 

  13070   Fri Jun 16 18:21:40 2017 jigyasaConfigurationCamerasGigE camera IP

One of the additional GigE cameras has been IP configured for use and installation. 

Static IP assigned to the camera- 192.168.113.152
Subnet mask- 255.255.255.0
Gateway- 192.168.113.2
 

  13069   Fri Jun 16 13:53:11 2017 gautamUpdateCDSslow machine bootfest

Reboots for c1psl, c1iool0, c1iscaux today. MC autolocker log was complaining that the C1:IOO-MC_AUTOLOCK_BEAT EPICS channel did not exist, and running the usual slow machine check script revealed that these three machines required reboots. PMC was relocked, IMC Autolocker was restarted on Megatron and everything seems fine now.

 

  13068   Fri Jun 16 12:37:47 2017 Kaustubh, JigyasaUpdateComputersOttavia Switched On

Ottavia had been left running overnight and it seems to work fine. There has been no smell or any noticeable problems in the working. This morning Gautam, Kaustubh and I connected Ottavia to the Matrian Network through the Netgear switch in the 40m lab area. We were able to SSH into Ottavia through Pianosa and access directories. On the ottavia itself we were able to run ipython, access the internet. Since it seems to work out fine, Kaustubh and I are going to enable the ethernet connection to Ottavia and secure the wiring now.  

Quote:

It has been working fine the whole day(we didn't do much testing on it though). We are leaving it on for the night.

Quote:

Today, I and Jigyasa connected the Ottavia to one of the unused monitor screens Donatella. The Ottavia CPU had a label saying 'SMOKED''. One of the past elogs, 11091, dated back in March 2015, by Jenne had an update regarding the Ottavia smelling 'burny'. It seems to be working fine for about 2 hours now. Once it is connected to the Martian Network we can test it further. The Donatella screen we used seems to have a graphic problem, a damage to the display screen. Its a minor issue and does not affect the display that much, but perhaps it'll be better to use another screen if we plan to use the Ottavia in the future. We will power it down if there is an issue with it.

 

 

  13067   Thu Jun 15 19:49:03 2017 Kaustubh, JigyasaUpdateComputersOttavia Switched On

It has been working fine the whole day(we didn't do much testing on it though). We are leaving it on for the night.

Quote:

Today, I and Jigyasa connected the Ottavia to one of the unused monitor screens Donatella. The Ottavia CPU had a label saying 'SMOKED''. One of the past elogs, 11091, dated back in March 2015, by Jenne had an update regarding the Ottavia smelling 'burny'. It seems to be working fine for about 2 hours now. Once it is connected to the Martian Network we can test it further. The Donatella screen we used seems to have a graphic problem, a damage to the display screen. Its a minor issue and does not affect the display that much, but perhaps it'll be better to use another screen if we plan to use the Ottavia in the future. We will power it down if there is an issue with it.

 

  13066   Thu Jun 15 18:56:31 2017 jigyasaUpdateComputer Scripts / ProgramsMC2 Pitch-Yaw offset

A python script to randomly vary the MC2 pitch and yaw offset and correspondingly record the value of MC transmission has been started on Donatella in the control room and should run for a couple of hours overnight.

The script is named MC_TRANS_1.py and is located in my user directory at /users/jigyasa

Apologies for any inconvenience.
Data analysis will follow.

  13065   Thu Jun 15 14:24:48 2017 Kaustubh, JigyasaUpdateComputersOttavia Switched On

Today, I and Jigyasa connected the Ottavia to one of the unused monitor screens Donatella. The Ottavia CPU had a label saying 'SMOKED''. One of the past elogs, 11091, dated back in March 2015, by Jenne had an update regarding the Ottavia smelling 'burny'. It seems to be working fine for about 2 hours now. Once it is connected to the Martian Network we can test it further. The Donatella screen we used seems to have a graphic problem, a damage to the display screen. Its a minor issue and does not affect the display that much, but perhaps it'll be better to use another screen if we plan to use the Ottavia in the future. We will power it down if there is an issue with it.

  13064   Thu Jun 15 01:56:50 2017 gautamUpdateASSETMY Oplev restored

Summary:

I tried playing around with the Oplev loop shape on ITMY, in order to see if I could successfully engage the Coil Driver whitening. Unfortunately, I had no success tonight.

Details:

I was trying to guess a loop shape that would work - I guess this will need some more careful thought about loop shape optimization. I was basically trying to keep all the existing filters, and modify the low-passing that minimizes control noise injection. By adding a 4th order elliptic low pass with corner at 50Hz and stopband attenuation of 60dB yielded a stable loop with upper UGF of ~6Hz and ~25deg of phase margin (which is on the low side). But I was able to successfully engage this loop, and as seen in Attachment #1, the noise performance above 50Hz is vastly improved. But it also seems that there is some injection of noise around 6Hz. In any case, as soon as I tried to engage the dewhitening, the DAC output quickly saturated. The whitening filter for the ITMs has ~40dB of gain at ~40Hz already, so it looks like the high frequency roll-off has to be more severe.

I am not even sure if the Elliptic filter is the right choice here - it does have the steepest roll off for a given filter order, but I need to look up how to achieve good roll off without compromising on the phase margin of the overall loop. I am going to try and do the optimization in a more systematic way, and perhaps play around with some of the other filters' poles and zeros as well to get a stable controller that minimizes control noise injection everywhere.

Attachment 1: ITMY_OLspec.pdf
ITMY_OLspec.pdf
  13063   Wed Jun 14 18:15:06 2017 gautamUpdateASSETMY Oplev restored

I replaced the Pentek Generic Whitening Board and the Optical Lever PD Interface Board (D010033) which I had pulled out. The ETMY optical lever servo is operational again. I will post a more detailed elog with deviations from schematics + photos + noise and TF measurements shortly.

Quote:

As part of my Oplev servo investigations, I have pulled out the Pentek Generic Whitening board (D020432) from the Y-end electronics rack. ETMY watchdog was shutdown for this, I will restore it once the Oplev is re-installed.

 

  13062   Tue Jun 13 08:40:32 2017 SteveUpdateIMCIMC wonkiness

Happy MC after last glitch at 10:28 so the credit goes to Rana

GV edit 11:30am: I think the stuff at 10:28 is not a glitch but just the WFS servos coming on - the IMC was only hand aligned before this.

Quote:

It happened again. MC2 UL seems to have gotten the biggest glitch. It's a rather small jump in the signal level compared to what I have seen in the recent past in connection with suspect Satellite boxes, and LL and UR sensors barely see it.

I will squish Sat box cables and check the cabling at the coil driver board end as well, given that these are two areas where there has been some work recently. WFS loops will remain off till I figure this out. At least the (newly centered) DC spot positions on the WFS and MC2 TRANS QPD should serve as some kind of reference for good MC alignment.

GV edit 9pm: I tightened up all the cables, but doesn't seem to have helped. There was another, larger glitch just now. UR and LL basically don't see it at all (see Attachment #2). It also seems to be a much slower process than the glitches seen on MC1, with the misalignment happening over a few seconds (it is also a lot slower). I have to see if this is consistent with a glitch in the bias voltage to one of the coils which gets low passed by a 4xpole@1Hz filter.

Quote:

Once we had the beam approximately centered for all of the above 3 PDs, we turned on the locking for IMC, and it seems to work just fine. We are waiting for another hour for switching on the angular allignment for the mirrors to make sure the alignment holds with WFS turned off.

 

 

Attachment 1: happy_MC.png
happy_MC.png
Attachment 2: last_glitch.png
last_glitch.png
  13061   Mon Jun 12 22:23:20 2017 ranaUpdateIMCIMC wonkiness

wonder if its possible that the slow glitches in MC are just glitches in MC2 trans QPD? Steve sometimes dances on top of the MC2 chamber when he adjusts the MC2 camera.

I've re-enabled the WFS at 22:25 (I think Gautam had them off as part of the MC2 glitch investigation). WFS1 spot position seems way off in pitch & yaw.

From the turn on transient, it seems that the cross-coupled loops have a time constant of ~3 minutes for the MC2 spot, so maybe that's not consistent with the ~30 second long steps seen earlier.

ELOG V3.1.3-