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ID Date Author Type Category Subjectup
  8911   Tue Jul 23 19:38:58 2013 gautamUpdateCDSCharacterisation of DAC at 1X9

 

 I just finished carrying out the same checks for the DAC at 1X9 (with channels 9 through 16 that are unused as of now) as those I had done for the DAC at 1Y4, as the hardware prep up till now was done with the characterisation of the DAC at 1Y4. Conclusions:

  • The accessible range of output voltage are -10 V to +10V w.r.t ground --> No change needs to be made to the gain of the HV amplifier stage on the PZT Driver Board
  • The pin-outs of the DAC Adaptor Board at 1X9 is identical to that at 1Y4 --> Custom ribbons do not need to be modified.
  • The PSD of the DAC output has a peak at 64 kHz --> Notches on AI Board do not need to be moved again.

I will now proceed to install various pieces of hardware (AI Board, PZT driver board, HV Power Supply and cabling) at 1X9, while not making the connection to the PZTs till I receive the go ahead. 

  3197   Mon Jul 12 15:49:56 2010 nancyUpdateSUSCharacterisation of the QPD

I and koji setup the measurement of the QPD response to the pitch and yaw displacements of the beam spot.

We did this using a 100mW 1064nm laser. Its power was attenuated to ~ 1.9mW, and the spot size at the QPD position was 6000-7000 um .

The QPD was put on a translation stage, using which, the center of teh QPD wrt the beam spot could be moved in pitch and yaw.

Following are the measurements :

For yaw

:fullyaw.jpg

The slope of teh linear region is -8356 /inch

yaw_linear.jpg

 For pitch

fullpitch.jpg

The slope of the linear region in this is 9085/inch

 

pitch_linear.jpg

 

  3198   Mon Jul 12 17:05:30 2010 nancyUpdateSUSCharacterisation of the QPD

Quote:

I and koji setup the measurement of the QPD response to the pitch and yaw displacements of the beam spot.

We did this using a 100mW 1064nm laser. Its power was attenuated to ~ 1.9mW, and the spot size at the QPD position was 6000-7000 um .

The QPD was put on a translation stage, using which, the center of teh QPD wrt the beam spot could be moved in pitch and yaw.

Following are the measurements :

 

 The old plots looked horrible, and so here is a new plot

plot.png

The slopes and other stats are

Pitch

Linear model Poly1:
     f(x) = p1*x + p2
Coefficients (with 95% confidence bounds):
       p1 =        8550  (7684, 9417)
       p2 =       -2148  (-2390, -1906)

Goodness of fit:
  SSE: 9944
  R-square: 0.9923
  Adjusted R-square: 0.9907
  RMSE: 44.59

Yaw

Linear model Poly1:
     f(x) = p1*x + p2
Coefficients (with 95% confidence bounds):
       p1 =       -8310  (-8958, -7662)
       p2 =        2084  (1916, 2252)

Goodness of fit:
  SSE: 6923
  R-square: 0.9954
  Adjusted R-square: 0.9945
  RMSE: 37.21

Attachment 1: plot.png
plot.png
  14111   Sat Jul 28 22:16:49 2018 John MartynUpdate Characterization of Transimpedance Amplifier

Kevin and I meaured the transfer function of the photodiode circuit using the Jenne laser and agilent in the 40m lab. The attached figures depict our measured transfer function over the modulation frequency ranges of 30kHz-30MHz and 1kHz-30MHz when the power of the laser was set to 69 and 95 μW. These plots indicate a clear roll off frequency around 300 kHz. In addition, the plots beginning at 1kHz display unstable behavior at frequencies below 30kHz. I am not sure why there is such a sharp change in the transfer function around 30kHz, but I suspect this to be due to an issue with the agilent or photodiode. 

Attachment 1: PD_TF1.pdf
PD_TF1.pdf
Attachment 2: PD_TF2.pdf
PD_TF2.pdf
Attachment 3: PD_and_TIA_Transfer_Function_Measurements.zip
  14112   Sun Jul 29 00:59:54 2018 KojiUpdateElectronicsCharacterization of Transimpedance Amplifier

You have this measurement problem when the IF bandwidth is larger than the measurement frequency. I suspect the IF bandwidth is 30kHz.

  10036   Fri Jun 13 11:33:55 2014 AkhilUpdateElectronicsCharacterization of UFC-6000 RF Frequency Counter

 Goal:

To characterize the Mini-Circuits RF FC (Model UFC-6000) and plot Bode Plots at varying Modulation frequencies.

Work Done:

Here are the list of measurements(files attached) taken from FC using SRS(Model DS345) Synthesized Function Generator for a Sinusoidal signal at different Modulation Frequencies ranging from 0.01 Hz to 1 KHz:

Carrier Frequency                          Modulation Depth                                                        Attached measurement Folder 

5 MHz                                                     Δ f = 5 MHz                                                                            Bode_5

10 MHz                                                   Δ f = 10 MHz                                                                          Bode_10

20 MHz                                                   Δ f = 20 MHz                                                                           Bode_20 

 

The measured data will be used to estimate:

1) Transfer Function of FC 

2) Quantization noise from Power Spectral Density(PSD) vs Hz

 

To Do Next:

1)Complete interfacing the Pi with EPICS.

2)Make bode plots (Matlab script attached) and PSD plots and estimate the control parameters for optimal design of FOLL PID loop.

 

 

Attachment 1: Bode_Plots.zip
  10238   Fri Jul 18 17:10:57 2014 NichinSummaryElectronicsCharacterization of demodulator boards.

Rack 1Y2, I took transfer function measurements for each of the following demodulator boards: REFL11, REFL33, REFL55, REFL165, AS55, POP22, POX11 and POY11.

What I did:

1) Removed the wire at PD Input to demodulator board.

2) Put the MOD output from network analyzer into PD input of board.

3) Ran a sweep from 100kHz to 100MHz.

4) Measured the transfer function between PD RF MON and PD Input. (The PD RF MON signal came out of the RF multiplexer, so the mux is included as well )

5) Put the original wire back at PD Input.

Results:

The plots clearly show an attenuation of 20dB (factor of 10) for all the demodulator boards. This explains why my transimpedance measurements are off by 10 times.

Note: for REFL 165, there was an extra 100MHz high pass filter installed at PD Input. I did not remove this and made my measurements along with this.

To Do:

a) Modify the PDFR system to calibrate out this attenuation.

b) Measure the transfer function between the input and output of RF mux, so that we can have just the transfer function between PD input an PD RF MON (for documentation's sake)

 

Attachment 1: Demodulators_TF.pdf
Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf
  10252   Tue Jul 22 15:50:35 2014 NichinSummaryElectronicsCharacterization of demodulator boards.

Quote:

Rack 1Y2, I took transfer function measurements for each of the following demodulator boards: REFL11, REFL33, REFL55, REFL165, AS55, POP22, POX11 and POY11.

What I did:

1) Removed the wire at PD Input to demodulator board.

2) Put the MOD output from network analyzer into PD input of board.

3) Ran a sweep from 100kHz to 100MHz.

4) Measured the transfer function between PD RF MON and PD Input. (The PD RF MON signal came out of the RF multiplexer, so the mux is included as well )

5) Put the original wire back at PD Input.

Results:

The plots clearly show an attenuation of 20dB (factor of 10) for all the demodulator boards. This explains why my transimpedance measurements are off by 10 times.

Note: for REFL 165, there was an extra 100MHz high pass filter installed at PD Input. I did not remove this and made my measurements along with this.

To Do:

a) Modify the PDFR system to calibrate out this attenuation.

b) Measure the transfer function between the input and output of RF mux, so that we can have just the transfer function between PD input an PD RF MON (for documentation's sake)

 

I repeated the exact steps above and made sure everything was back where it should be after I was done.

Reason I had to retake the measurements:

My script for acquiring data from the AG4395A network analyzer was such that it first acquired the magnitude data from channel 1 and then recorded phase data from channel 2 without holding its trace. Hence the phase and magnitude data were not exactly in sync with each other. So, when I tried to fit the data to a model using vector fitting, I ended up with very bad results.

I have now changed every single script relating to the network analyzer to just get the real and imaginary data in one go and then calculate the phase using this data.

The fitting process is now in progress and results will be up shortly.

Attachment 1: Demodulators_TF.pdf
Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf Demodulators_TF.pdf
  10263   Wed Jul 23 11:54:27 2014 NichinUpdateElectronicsCharacterization of demodulator boards.

Quote:

 

I repeated the exact steps above and made sure everything was back where it should be after I was done.

Reason I had to retake the measurements:

My script for acquiring data from the AG4395A network analyzer was such that it first acquired the magnitude data from channel 1 and then recorded phase data from channel 2 without holding its trace. Hence the phase and magnitude data were not exactly in sync with each other. So, when I tried to fit the data to a model using vector fitting, I ended up with very bad results.

I have now changed every single script relating to the network analyzer to just get the real and imaginary data in one go and then calculate the phase using this data.

The fitting process is now in progress and results will be up shortly.

The plots in the previous Elog includes delay and a little attenuation by RF cables and the RF mux.

Today I separately calculated the delay and attenuation for an RG405 cable (550 cm) and the RF mux(using really small RF cables). These delays should be accounted for when fitting the transfer function of Demodulator boards and transimpedance of PDs.

The plots are in both semilogx and linear.

Attachment 1: 1.pdf
1.pdf 1.pdf
Attachment 2: 2.pdf
2.pdf 2.pdf
  5849   Wed Nov 9 14:49:07 2011 kiwamuSummaryLSCCharacterization of the Power Recycled Michelson

EDIT by KI:

  The definition of the recycling gain is wrong here.

See the latest entry (#5875)

 

Here is a summary about the Power Recycled Michelson (PRMI).

It seems the mode matching is also one of the greatest contributor on the low recycling gain.

 

 

 (Estimated parameters)

    Loss = 5.3% (or effective reflectivity of  93.28% in Michleson) => Under coupling !!

     +  Mode matching efficiency = 47.4 %  => Really bad !!

   With these values we end up with a recycling gain of 7 and a normalized REFLDC of  0.5 as observed (#5773).

Also according the incident beam scan measurement (#5773) the loss is NOT a local effect like a clipping, it is more like uniformly distributed thing.

As for the mode matching, the number indicates that approximately the half of the incident light is coming back to the REFL port without interacting with PRMI.

This is bad because the non-mode-matched light, which is just a junk light, is entering into the photo detectors unnecessarily.

In the worst scenario, those junk light may create a funny signal, for example a signal sensitive to the alignment of PRM.

 

(Estimation method)

The method to estimate the loss and the MM (Mode-Matching efficiency) is essentially the same as before (#5541).

One difference from the previous estimation is that the I used more realistic parameters on the transmissivity of ITMs and PRM :

     PRM : T = 5.637 %  (see the 40m wiki)

     ITM : T = 1.384 %  (see the 40m wiki)

 

 In addition to the basic calculations I also made plots which are handy for figuring out where we are.

Quantities we can measure are the reflected light from PRMI and the recycling gain using the REFL PD and the POY PD respectively.

So I wanted to see how the loss and MM can be estimated from the measured REFL DC and recycling gain.

The plots below are the ones.

contour_loss.png   contour_MM.png

[Loss map]

 The first figure shows a contour map of the loss as a function of the measured REFL DC and recycling gain.

The white area is a place where no proper solutions can be found (for example MM can get to more than 100 or loss becomes negative).

The star mark in the plot corresponds to the place where we are now. Obviously the loss is about 5%.

If we somehow decrease the amount of the loss the star mark will mostly go up in the plot.

[MM map]
 The second figure shows a contour map of the MM as a function of the measured REFL DC and recycling gain. 

The X and Y axis are exactly the same as that of the first plot. Again the star mark represents the place where we are.

We are currently at MM=47%

 

(Solutions)

Here are some solutions to bring the recycling gain higher.

We don't work on these things immediately since it requires opening of the chambers again and it will take some times.

But we should think about those options and prepare some stuff for a coming vent.

  + Refinement of the position of the mode matching telescopes.  => The Recycling gain can go up to 15.

     => Assuming the loss in the cavity doesn't change, the star mark in the first plot will go to the left hand side along the "0.05" black solid line.

     => However PRMI will be still under coupled.

     => Needs an estimation about which way we move the telescopes.

 + Locate the place of the dominant loss source and reduce it somehow.

    => The recycling gain will be more than 18 if the loss reduces by a factor of more than 5.

    => Needs a clever way to find it otherwise we have to do it in the classical way (i.e. white light and trying to find dirty surfaces)

  5851   Wed Nov 9 16:29:36 2011 KojiSummaryLSCCharacterization of the Power Recycled Michelson

Difficult to understand.

The mode matching does not change the recycling gain. It changes the coupling of the incident light into the cavity.
It changes the reflected and accumulated power, but the recycling gain is not affected.

The recycling gain is determined by the optical configuration and the optical loss in the cavity.

In the actual measurement, of course, we should take both of the loss and the mode matching into account.
But this is the issue of the measurement method.

The essential questions are:
How much is the actual recycling gain? And how does it affect the signal extraction?

  5875   Fri Nov 11 14:55:47 2011 kiwamuSummaryLSCCharacterization of the Power Recycled Michelson : take 2

Quote from #5851

The recycling gain is determined by the optical configuration and the optical loss in the cavity.

How much is the actual recycling gain? And how does it affect the signal extraction?

 As Koji pointed out I made a wrong definition on the recycling gain of PRMI (Power-Recycled Michelson Interferomter).

In the correct definition the estimated recycling gain is 15.
In order to answer Koji's second question,which is about the effect on the signal extraction,
I need to scratch my head for a while.
( Give me some time..)
 
The value what I called "Recycling gain" must have been called "measured power build up" or something like that.
For clarity I put the definitions of the quantities.
    Recycling gain :      rec_gain.png 

   Reflectivity of PRMI (measured by REFLDC): refl.png

    Power build up (measured by POY DC) : pbu.png

    Mode Matching (MM) efficiency :  MM.png

    Loss in the PRMI cavity : loss.png

 


 (Results of Measurement and Estimation)

     Estimated recycling gain = 15

     Estimated MM efficiency = 47.4%

     Estimated Loss = 5.3%

     Measured power build Up = 7

     Measured reflectivity of PRMI = 0.5

  3419   Fri Aug 13 09:41:00 2010 nancyOmnistructureComputersCharger for dell laptop

 I have taken the charger for the dark gray dell laptop from its station, and have labelled the information there too.

Will keep it back tonight.

  16196   Wed Jun 9 18:29:13 2021 Anchal, PacoSummaryALSCheck for saturation in ITMX SOS Driver

We did a quick check to make sure there is no saturation in the C1:SUS-ITMX_LSC_EXC analog path. For this, we looked at the SOS driver output monitors from the 1X4 chassis near MC2 on a scope. We found that even with 600 x 10 = 6000 counts of our 619 Hz excitation these outputs in particular are not saturating (highest mon signal was UL coil with 5.2 Vpp). In comparison, the calibration trials we have done before had 600 counts of amplitude, so we can safely increase our oscillator strength by that much yes


Things that remain to be investigated -->

  • What is the actual saturation level?
  • Two-tone intermodulation?
  14060   Thu Jul 12 21:16:25 2018 aaronUpdateOMCChecking OMC Electronics

In preparation for tomorrow's vent, I'm checking some of the OMC-related electronics we plan to use.

First up is the HV Piezo Driver (D060283).

(well, technically the first up was the Kepco HV power supply... but I quickly tested that its output works up to 300V on a multimeter. The power supply for OMC-L-PZT is all good!)

According to the DCC, the nominal HV supply for this board is 200V; the board itself is printed with "+400V MAX", and the label on the HV supply says it was run at 250V. For now I'm applying 200V. I'm also supplying +-15V from a Tektronix supply.

I used two DB25 breakout boards to look at the pins for the DC and AC voltage monitors (OMC_Vmon_+/-, pins 1/6, and OMC_Vmon_AC+/-, pins 2 and 7) on a scope. I hooked up a DS345 function generator to the piezo drive inputn (pins 1,6). According to the 2013 diagram from the DCC, there is just one drive input, and an alternative "dither in" BNC that can override the DAC drive signal. I leave the alternative dither floating and am just talking to the DAC pins.

Aspects of the system seem to work. For example, I can apply a sine wave at the input, and watch on the AC monitor FFT as I shift the frequency. However, anything I do at DC seems to be filtered out. The DC output is always 150V (as long as 200V comes from the supply). I also notice that the sign of the DC mon is negative (when the Vmon_+ pin is kept high on the scope), even though when I measure the voltage directly with a multimeter the voltage has the expected (+) polarity.

A few things to try:

  • The DC_Readout electronics scheme on the wiki has separate oscillator and control inputs. This diagram has lied to us in the past and is older, and the traces on top of the breadboard seem to only go to pins 1 and 6, but I'm going to first try to apply a voltage across pins 2 and 7 in case there actually is a separate control I'm ignoring.
    • Driving on these pins seems to do nothing

On further investigation this was the key clue. I had the wrong DCC document, this is an old version of this board, the actual board we are using is version A1 of D060283-x0 (one of the "other files")

Gautam and Koji returned at this point and we started going through the testpoints of the board, before quickly realizing that the DC voltage wasn't making it to the board. Turns out the cable was a "NULL" cable, so indeed the AC wasn't passing. We swapped out the cable, and tested the circuit with 30V from the HV supply to trim the voltage reference at U14. The minimum voltage we could get is 5V, due to the voltage divider to ground made by R39. We confirmed that the board, powered with 200V, can drive a sine wave and the DC and AC mons behave as expected.

  14072   Sat Jul 14 16:04:34 2018 aaronUpdateOMCChecking OMC Electronics

Next check is the DCPD/OMMT Satellite Box

I traced a cable from the OMC electrical feedthrough flanges to find the DCPD/OMMT Satellite Box (D060105). I couldn't find the DCC number or mention of the box anywhere except this old elog.

Gautam and I supplied the box with power and tested what we think is the bias for the PD, but don't read any bias... we tracked down the problem to a suspicious cable, labelled.

We confirmed that the board supplies the +5V bias that Rich told us we should supply to the PDs.

We tested the TFs for the board from the PD input pins to output pins with a 100kHz low pass (attached, sorry no phase plots). The TFs look flat as expected. The unfiltered outputs of the board appear bandpassed; we couldn't identify why this was from the circuit diagram but didn't worry too much about it, as we can plan to use the low passed outputs.

Attachment 1: Screenshot_2018-07-14_17.53.40.png
Screenshot_2018-07-14_17.53.40.png
Attachment 2: Screenshot_2018-07-14_17.57.17.png
Screenshot_2018-07-14_17.57.17.png
  4904   Tue Jun 28 22:36:04 2011 JamieUpdateSUSChecking binary switching of SUS whitening filter

I have been checking the binary output switching for the SUS whitening filters. It appears that the whitening switching is working for (almost) all the vertex suspensions (BS, ITMX, ITMY, PRM, SRM), but not for the ETMs.

The table below lists the output from my switch-checking script (attached). The script uses the SUS digital lockin to drive one coil and measure the same coil's OSEM response, repeating for each coil/OSEM pair. I used a lockin drive frequency of about 10 Hz, at which the whitening filter should have 10 db of gain.

All but one of the vertex OSEMS show the proper response (~10db gain at 10Hz) when the whitening is switched on from the digital controls. ITMY UL appears to not be switching, which I fear is due to my electronics fail noted in my previous log post.  The ETMs are clearly not switching at all.

I will try to get the ETM switching working tomorrow, as well as try to asses what can be done about the ITMY UL switch.  After that I will work on confirming the coil drive dewhite switching.

lockin settings

freq: 10.123 Hz
amp: 10000
I/Q filters: 0.1 Hz LP, 4-pole butterworth

response

BS
ul : 3.31084503062 = 10.3987770676 db
ll : 3.34162124753 = 10.4791444741 db
sd : 3.43226254574 = 10.7116100229 db
lr : 3.28602651913 = 10.3334212798 db
ur : 3.29361593249 = 10.3534590969 db

ITMX
ul : 3.37499773336 = 10.5654697099 db
ll : 3.2760924572  = 10.3071229966 db
sd : 3.13374799272 =  9.9212813757 db
lr : 3.28133776018 = 10.3210187243 db
ur : 3.37250879937 = 10.5590618297 db

ITMY
ul : 0.99486434364 = -0.0447226830807 db
ll : 3.39420873724 = 10.6147709414 db
sd : 3.88698713176 = 11.7922620572 db
lr : 3.357123865   = 10.5193473069 db
ur : 3.37876008179 = 10.5751470918 db

PRM
ul : 3.26758918055 = 10.2845489876 db
ll : 3.32023820566 = 10.4233848529 db
sd : 3.25205538857 = 10.2431586766 db
lr : 3.24610681962 = 10.227256141  db
ur : 3.31311970305 = 10.4047425446 db

SRM
ul : 3.30506423619 = 10.3835980943 db
ll : 3.28152094133 = 10.3215036019 db
sd : 3.08566647696 =  9.7869796462 db
lr : 3.30298270419 = 10.378125991  db
ur : 3.3012249406  = 10.3735023505 db

ETMX
ul : 0.99903400106 = -0.00839461539757 db
ll : 0.99849991349 = -0.0130393683795 db
sd : 1.00314092883 =  0.0272390056874 db
lr : 1.00046493718 =  0.00403745453682 db
ur : 1.00265600785 =  0.0230392084558 db

ETMY
ul : 1.00223179107 =  0.0193634913327 db
ll : 0.96755532811 = -0.286483823189 db
sd : 1.00861855271 =  0.0745390477589 db
lr : 1.05718545676 =  0.483023602007 db
ur : 0.99777406174 = -0.0193558045143 db
Attachment 1: botest.py
#!/usr/bin/env python

import sys
import os
import subprocess
import time
import pickle
from numpy import *
import nds
import matplotlib
... 207 more lines ...
  696   Fri Jul 18 17:12:35 2008 JenneUpdateIOOChecking out the MC Servo Board
[Jenne, Max]

One of the things that Rana thinks that might be causing my MC_F calibration to be off is that the MC Servo Board's filters don't match those on the schematics. Max and I pulled the MC servo board today to check resistor and capacitor values. Alberto needed the Mode Cleaner, so we put the board back before finishing checking values. We will probably pull the board again next week to finish checking the values.

I haven't checked to ensure that the MC still locks, because Yoichi is doing stuff on the PSL table, but I didn't change anything on the board, and hooked all the cables back where they were, so hopefully it's all okay.
  697   Fri Jul 18 19:15:15 2008 JenneUpdateIOOChecking out the MC Servo Board

Quote:
[Jenne, Max]

I haven't checked to ensure that the MC still locks, because Yoichi is doing stuff on the PSL table, but I didn't change anything on the board, and hooked all the cables back where they were, so hopefully it's all okay.


I put the PMC back and the MC now locks.
  11603   Tue Sep 15 20:44:13 2015 gautamSummaryLSCChecking the delay line phase shifter DS050339
I checked out the delay line phase shifter D050339, (theory of operation here) this afternoon. I first checked that the power connection was functional, which it was, though the power connector is is not the usual chassis one (see image attached, do we need to change this?).

The box has two modes of operation - you can either change the delay by flipping switches on the front panel or via a 25pin D-sub connector on the back (the pin numberings for this connector on the datasheet are a little misleading, but I determined that pins 1-9 on the D-sub connector correspond to the 9 delays on the front panel in ascending order, pin 10 is the mode selector switch, should be high for remote operation, pins 11 and 13 are NC, pin 12 is VCC of 5V, and pins 14-25 are grounded). I first checked the front-panel mode of operation, using an oscilloscope to measure the delay between the direct signal from the Fluke 6061 and the output from the D050339. This corresponds to the first set of datapoints in the plot attached (signal was 100MHz sine wave).

I then used a 25 pin D sub breakout boards to check the remote operation mode as well, which corresponds to the second set of datapoints in the plot attached. For this measurement, I used the Agilent network analyzer to measure the phase lag between the direct signal (for all delays, I measured the phase lag at 100MHz, having first calibrated the "thru" path by connecting the R and A inputs of the network analyzer using a barrel BNC) and the delayed output from the box, and then converted it to a time delay.

Both sets of data are linear, with a slope nearly equal to 1 as expected. I conclude that the box is functioning as expected. Right now, Koji is checking a board which will be used to remotely control this box. On the hardware side it remains to make a cable going from the DS050339 Dsub input to the driver board output (also 25 pin Dsub).
Attachment 1: IMG_20150915_193100.jpg
IMG_20150915_193100.jpg
Attachment 2: Calibration.pdf
Calibration.pdf
  16442   Mon Nov 1 14:51:34 2021 KojiUpdateGeneralChecking the vent plan

The vent team described a detailed vent plan (and reports where the actions have been performed)

https://wiki-40m.ligo.caltech.edu/vent/Fall2021

- [Sec.4] We should decide the final PR2 mirror through table-top measurements.

- [Sec 6] BS alignment is probably "unknown" now. So it'd be better to use the ITMY spot as the reference, then align BS for ITMX. For temporary alignment, it's OK though.

- [Sec 9-11] RIght now there is no mounts to place LO3/LO4/AS2/AS3/BHDBS. But we probably want to test something before the installation of the BHD? Just place the BHDBS on a optics mount so that we get an interfered beam on ITMY?

At this point we are supposed to have all the electronics all the CDS necessary for the new SOS control. Otherwise, they are just swinging and the alignment work will just be impossible.

- [Sec 15] The OPLEV mirrors can be freely moved as long as it does not block the main IR beams. Moving ITMXOL1 makes the reflection blocked by ITMXOL2. And moving ITMXOL2 would make the IR beams clipped. Consider replacing the mounts with a fixed mount. (The OPLEV mirrors are 1.5" in dia. It is not common vacuum compatible 1.5inch mounts. If 1" Al mirror is sufficient, we can use it.

https://wiki-40m.ligo.caltech.edu/vent/Fall2021/FinalAlignment

- The arms are the most strict alignment requirement. Everything else will follow the arm alignment. So start from the arms and propagate the alignment to Michelson / PRMI / SRMI.

- We reestablish arm alignment using the end green beams.

- Then recover IR arm alignment. Consider using ASS if possible

  2762   Sun Apr 4 00:21:42 2010 rana, kojiSummaryElectronicsCheckout of EG&G (PARC) preamp model #113, s/n 49135

We tested out the functionality of the EG&G 113 preamp that I found in one of the cabinets. This is one of the ancestors of the SR560 preamp that we are all used to.

It turns out that it works just fine (in fact, its better than the SR560). The noise is below 3nV/rHz everywhere above 30 Hz. The filter settings from the front panel all seem to work well. And the red knob on the front panel allows for continuous (i.e. not steps) gain adjustment. In the high-bandwidth mode (low pass filter at 300 kHz), there is ~35 deg of phase lag at 100 kHz. So the box is pretty fast.

IMG_0628.JPG

I would easily recommend this above the SR560 for use in all applications where you don't need to drive a 50 Ohm load. Also the battery is still working after 17 years!

There's several more of the this vintage in one of the last cabinets down the new Y-arm.

  15543   Wed Aug 26 22:49:47 2020 gautamUpdateElectronicsCheckout of Trek Model 603

I unboxed the Trek amplifier today, and performed some basic tests of the functionality. It seems to work as advertised. However, we may have not specified the correct specifications - the model seems to be configured to drive a bipolar output of +/- 125 V DC, whereas for PZT driving applications, we would typically want a unipolar drive signal. From reading the manual, it appears to me that we cannot configure the unit to output 0-250V DC, which is what we'd want for general PZT driving applications. I will contact them to find out more. 

The tests were done using the handheld precision voltage source for now. I drove the input between 0 to +5 V and saw an output voltage (at DC) of 0-250 V. This is consistent with the voltage gain being 50V/V as is stated in the manual, but how am I able to get 250 V DC output even though the bipolar configuration is supposed to be +/- 125 V? On the negative side, I am able to see 50V/V gain from 0 to -1 V DC. At which point making the input voltage more negative does nothing to the output. The unit is supposed to accept a bipolar input of +/- 10 V DC or AC, so I'm pretty sure I'm not doing anything crazy here...

Update:

Okay based on the markings on the rear panel, the unit is in fact configured for unipolar output. What this means is we will have to map the +/- 10 V DC output from the DAC to 0-5 V DC. Probably, I will stick to 0-2.5 V DC for a start, to not exceed 125 V DC to the PI PZT. I'm not sure what the damage spec is for that. The Noliac PZT I think can do 250 V DC no problem. Good thing I have the inverting summing amplifier coming in tomorrow...

Attachment 1: IMG_8951.JPG
IMG_8951.JPG
  11579   Fri Sep 4 20:42:14 2015 gautam, ranaUpdateCDSCheckout of the Wenzel dividers

Some years ago I bought some dividers from Wenzel. For each arm, we have x256 and a x64 divider. Wired in series, that means we can divide each IR beat by 2^14.

The highest frequency we can read in our digital system is ~8100 Hz. This corresponds to an RF frequency of ~132 MHz which as much as the BBPD could go, but less than the fiber PDs.

Today we checked them out:

  1. They run on +15V power.
  2. For low RF frequencies (< 40 MHz) the signal level can be as low as -25 dBm.
  3. For frequencies up to 130 MHz, the signal should be > 0 dBm.
  4. In all cases, we get a square wave going from 0 ~ 2.5 V, so the limiter inside keeps the output amplitude roughly fixed at a high level.
  5. When the RF amplitude goes below the minimum, the output gets shaky and eventually drops to 0 V.

Since this seems promising, we're going to make a box on Monday to package both of these. There will one SMA input and output per channel.

Each channel will have a an amplifier since this need not be a low noise channel. The ZKL-1R5 seems like a good choice to me. G=40 dB and +15 dBm output.

Then Gautam will make a frequency counter module in the RCG which can do counting with square waves and not care about the wiggles in the waveform.

I think this ought to do the trick for our Coarse frequency discriminator. Then our Delay Box ought to be able to have a few MHz range and do all of the Fast ALS Carm that we need.

Attachment 1: TEK00000.PNG
TEK00000.PNG
Attachment 2: TEK00001.PNG
TEK00001.PNG
Attachment 3: TEK00002.PNG
TEK00002.PNG
  11307   Tue May 19 11:15:09 2015 ericqUpdateComputer Scripts / ProgramsChiara Backup Hiccup

Starting on the 14th (five days ago) the local chiara rsync backup of /cvs/cds to an external HDD has been failing:

caltech/c1/scripts/backup/rsync_chiara.backup.log:

2015-05-13 07:00:01,614 INFO       Updating backup image of /cvs/cds
2015-05-13 07:49:46,266 INFO       Backup rsync job ran successfully, transferred 6504 files.
2015-05-14 07:00:01,826 INFO       Updating backup image of /cvs/cds
2015-05-14 07:50:18,709 ERROR      Backup rysnc job failed with exit code 24!
2015-05-15 07:00:01,385 INFO       Updating backup image of /cvs/cds
2015-05-15 08:09:18,527 ERROR      Backup rysnc job failed with exit code 24!
...
 

Code 24 apparently means "Partial transfer due to vanished source files."

Manually running the backup command on chiara worked fine, returning a code of 0 (success), so we are backed up. For completeness, the command is controls@chiara: sudo rsync -av --delete --stats /home/cds/ /media/40mBackup

Are the summary page jobs moving files around at this time of day? If so, one of the two should be rescheduled to not conflict. 

  11327   Wed May 27 15:20:54 2015 ericqUpdateComputer Scripts / ProgramsChiara Backup Hiccup

The local chiara backups are still failing due to vanished source files. I've emailed Max about the summary page jobs, since I think they're running remotely. 

  11336   Fri May 29 11:28:42 2015 ericqUpdateComputer Scripts / ProgramsChiara Backup Hiccup

I've changed the chiara local backup script to read a folder exclusion file, and excluded /users/public_html/detcharsummary, and things are working again. 

This was neccesary because the summary pages are being updated every half hour, which is faster than the time it takes for the backup script to run, so the file index that it builds at the start becomes invalid later on in the process. 


Thinking about chiara's disk, it strikes me that when we went from the linux1 RAID to a single HDD on chiara, we may have tightened a bottleneck on our NFS latency, i.e. we are limited to that single hard drive's IO rates. This of course isn't the culprit for the more recent dramatic slowdowns, but in addition to fixing whatever has happened more recently, we may want to consider some kind of setup with higher IO capability for the NFS filesystem. 

  11337   Fri May 29 12:49:53 2015 KojiUpdateComputer Scripts / ProgramsChiara Backup Hiccup

In fact, the file access is supposed to be WAY faster now than in the RAID case.

As noted in ELOG 9511, it was SCSI-2(or 3?) that had ~6MB/s thruput. Previously the backup took ~2hours.
This was improved to 30min by SATA HDD on llinux1.

I am looking at /opt/rtcds/caltech/c1/scripts/backup/rsync.backup.cumlog

In fact, this "30-min backup" was true until the end of March. After that the backup is taking 1h~1.5h.

This could be related to the recent NFS issue?

  11338   Fri May 29 15:12:39 2015 KojiUpdateComputer Scripts / ProgramsChiara Backup Hiccup

Actual data

Attachment 1: backup_hours.pdf
backup_hours.pdf
  16310   Thu Sep 2 20:44:18 2021 KojiUpdateCDSChiara DHCP restarted

We had the issue of the RT machines rebooting. Once we hooked up the display on c1iscex, it turned out that the IP was not given at it's booting-up.

I went to chiara and confirmed that the DHCP service was not running

~>sudo service isc-dhcp-server status
[sudo] password for controls:
isc-dhcp-server stop/waiting

So the DHCP service was manually restarted

~>sudo service isc-dhcp-server start
isc-dhcp-server start/running, process 24502
~>sudo service isc-dhcp-server status
isc-dhcp-server start/running, process 24502

 

 

  16311   Thu Sep 2 20:47:19 2021 KojiUpdateCDSChiara DHCP restarted

[Paco, Tega, Koji]

Once chiara's DHCP is back, things got much more straight forward.
c1iscex and c1iscey were rebooted and the IOPs were launched without any hesitation.

Paco ran rebootC1LSC.sh and for the first time in this year we had the launch of the processes without any issue.

  13154   Mon Jul 31 20:35:42 2017 KojiSummaryComputersChiara backup situation summary

Summary
- CDS Shared files system: backed up
- Chiara system itself: not backed up


controls@chiara|~> df -m
Filesystem     1M-blocks    Used Available Use% Mounted on
/dev/sda1         450420   11039    416501   3% /
udev               15543       1     15543   1% /dev
tmpfs               3111       1      3110   1% /run
none                   5       0         5   0% /run/lock
none               15554       1     15554   1% /run/shm
/dev/sdb1        2064245 1718929    240459  88% /home/cds
/dev/sdd1        1877792 1426378    356028  81% /media/fb9bba0d-7024-41a6-9d29-b14e631a2628
/dev/sdc1        1877764 1686420     95960  95% /media/40mBackup

/dev/sda1 : System boot disk
/dev/sdb1 : main cds disk file system 2TB partition of 3TB disk (1TB vacant)
/dev/sdc1 : Daily backup of /dev/sdb1 via a cron job (/opt/rtcds/caltech/c1/scripts/backup/localbackup)

/dev/sdd1 : 2014 snap shot of cds. Not actively used. USB

https://nodus.ligo.caltech.edu:8081/40m/11640

 

  13159   Wed Aug 2 14:47:20 2017 KojiSummaryComputersChiara backup situation summary

I further made the burt snapshot directories compressed along with ELOG 11640. This freed up additional ~130GB. This will eventually help to give more space to the local backup (/dev/sdc1)

controls@chiara|~> df -m
Filesystem     1M-blocks    Used Available Use% Mounted on
/dev/sda1         450420   11039    416501   3% /
udev               15543       1     15543   1% /dev
tmpfs               3111       1      3110   1% /run
none                   5       0         5   0% /run/lock
none               15554       1     15554   1% /run/shm
/dev/sdb1        2064245 1581871    377517  81% /home/cds
/dev/sdd1        1877792 1426378    356028  81% /media/fb9bba0d-7024-41a6-9d29-b14e631a2628
/dev/sdc1        1877764 1698489     83891  96% /media/40mBackup

 

 

  14385   Fri Jan 4 15:18:15 2019 KojiUpdateGeneralChiara disk clean up and internally mounted

[Koji Gautam]

Took the opprtunity of the power glitch to take care of the disk situation of chiara.

- Unmounted /cvs/cds from nodus. This did not affect the services on nodus as they don't use /cvs/cds

- Go to chiara, shut it down, and physically checked the labels of the drives.

root = 0.5TB
/cvs/cds = 4TB HGST
backup of /cvs/cds= 6TB HGST

- These three disks are internally mounted and connected with SATA. Previously, 6TB was on USB.

- There were two other drives (2TB and 3TB) but they seemed logically or physically broken. These two disks were removed from chiara. (they came back online after reformatting on mac. So they seem still physically alive).

controls@chiara|~> df
df: `/var/lib/lightdm/.gvfs': Permission denied
Filesystem      1K-blocks       Used  Available Use% Mounted on
/dev/sda1       461229088   10690932  427109088   3% /
udev             15915020          4   15915016   1% /dev
tmpfs             3185412        848    3184564   1% /run
none                 5120          0       5120   0% /run/lock
none             15927044        144   15926900   1% /run/shm
/dev/sdb1      5814346836 1783407788 3737912972  33% /media/40mBackup
/dev/sdc1      3845709644 1884187232 1766171536  52% /home/cds
controls@chiara|~> lsblk
NAME   MAJ:MIN RM   SIZE RO TYPE MOUNTPOINT
sda      8:0    0 465.8G  0 disk
├─sda1   8:1    0 446.9G  0 part /
├─sda2   8:2    0     1K  0 part
└─sda5   8:5    0  18.9G  0 part [SWAP]
sdb      8:16   0   5.5T  0 disk
└─sdb1   8:17   0   5.5T  0 part /media/40mBackup
sdc      8:32   0   3.7T  0 disk
└─sdc1   8:33   0   3.7T  0 part /home/cds
sr0     11:0    1  1024M  0 rom

- Rebooted the machine and just came back without any error. This time the control room machines were not shutdown, but they just recovered the NFS once chiara got back.

Attachment 1: P_20190104_143336.jpg
P_20190104_143336.jpg
Attachment 2: P_20190104_143357.jpg
P_20190104_143357.jpg
  10837   Tue Dec 23 14:33:24 2014 SteveUpdateVACChiara gets UPS

Quote:

Quote:

We had an unexpected power shutdown for 5 sec at ~ 9:15 AM.

Chiara had to be powered up and am in the process of getting everything else back up again.

Steve checked the vacuum and everything looks fine with the vacuum system.

PSL Innolight laser and the 3 units of IFO air conditions turned on.

The vacuum system reaction to losing power: V1 closed and Maglev shut down. Maglev is running on 220VAC so it is not connected to VAC-UPS.  V1 interlock was triggered by Maglev "failure" message.

Maglev was reset and started. After Chiara was turned on manually I could bring up the vac control screen through Nodus and opened V1

"Vacuum Normal" valve configuration was recovered instantly.

 

Chiara needs UPS 

It is arriving Thursday

 EricQ and Steve,

Steve preset the vacuum for safe-reboot mode with C1vac1 and C1vac2 running normal: closed valves as shown, stopped Maglev & disconnected valves V1 plus valves with moving labels.

(The position indicator of the valves changes to " moving " when its cable disconnected )

Eric shut down Chiara, installed APC's UPS Pro 1000 and restarted it.

All went well. Nothing unexpected happened. So we can conclude that the vacuum system with running C1vac1 and C1vac2 is not effected by Chiara's losing AC power.

Attachment 1: prepUP.png
prepUP.png
  11481   Thu Aug 6 01:38:19 2015 ericqUpdateComputer Scripts / ProgramsChiara gets new Ethernet card

Since Chiara's onboard ethernet card has a reputation to be flaky in Linux, Koji suggested we could just buy a new ethernet card and throw it in there, since they're cheap. 

I've installed a Intel EXPI9301CT ethernet card in Chiara, which detected it without problems. I changed over the network settings in /etc/networking/interfaces to use eth1 instead of eth0, restarted nfs and bind9, and everything looked fine. 

Sadly, EPICS/network slowdowns are still happening. :(

  11483   Thu Aug 6 09:16:57 2015 SteveUpdateVACChiara gets new Ethernet card
  1. Yesterday we did put the vacuum system into safe to reboot mode  for the ethernet card swap.
  2. Atm1, IFO pressure
  3. Atm2, as prepared valve configuration where " moving " means closed and disconnected

 

Attachment 1: ChiaraNetCard.png
ChiaraNetCard.png
Attachment 2: 23.png
23.png
  10835   Tue Dec 23 14:27:16 2014 ericqUpdateCDSChiara moved to UPS

 Steve and I switched chiara over to the UPS we bought for it, after ensuring the vacuum system was in a safe state. Everything went without a hitch. 

Also, Diego and I have been working on getting some of the new computers up and running. Zita (the striptool projecting machine) has been replaced. One think pad laptop is missing an HD and battery, but the other one is fine. Diego has been working on a dell laptop, too. I was having problems editing the MAC address rules on the martian wifi router, but the working thinkpad's MAC was already listed. 

  10836   Tue Dec 23 14:30:11 2014 ericqUpdateCDSChiara moved to UPS

Quote:

 Steve and I switched chiara over to the UPS we bought for it, after ensuring the vacuum system was in a safe state. Everything went without a hitch. 

Also, Diego and I have been working on getting some of the new computers up and running. Zita (the striptool projecting machine) has been replaced. One think pad laptop is missing an HD and battery, but the other one is fine. Diego has been working on a dell laptop, too. I was having problems editing the MAC address rules on the martian wifi router, but the working thinkpad's MAC was already listed. 

 Turns out that, as the martian wifi router is quite old, it doesn't like Chrome; using Firefox worked like a charm and now also giada (the Dell laptop) is on 40MARS.

  13977   Sun Jun 17 14:20:35 2018 KojiUpdateGeneralChiara new USB 4TB DIsk

I have connected a 4TB disk to chiara via a USB-SATA adapter. This disk has been recognized as /dev/sde. A GUID Partition Table (GPT), not MBR was made with gdisk to make a partition with the size beyond 2TB.
I tried to use "dd" to copy /home/cds (/dev/sdb1) to /dev/sde1, but failed. The copy was done (taking ~12h) and the partition was not recognized as a complete filesystem.

So I decided to use rsync instead.

sudo mkfs -t ext4 /dev/sde1
sudo mkdir /media/usb4g
sudo mount -t ext4 -o rw /dev/sde1 /media/usb4g
sudo rsync -a --progress /home/cds/ /media/usb4g

Progress
14:33 Copied     33G/1831G
14:38 Copied     36G/1831G
17:02 Copied   365G/1831G (~2.2GB/min)
01:18 Copied 1449G/1831G (~2.2GB/min)
04:36 Completed
> sent 1907955222607 bytes  received 126124609 bytes  37010956.31 bytes/sec
> total size is 1907271994803  speedup is 1.00

  13980   Mon Jun 18 12:07:03 2018 KojiUpdateGeneralChiara new USB 4TB DIsk

The initial local backup with rsync was done. Now the new 4TB disk is (supposed to be) automatically mounted at boot as /media/40mBackup so that we can run the daily backup on this disk. (<- This was confirmed by "sudomount -a")

controls@chiara|~> sudo blkid
...
/dev/sde1: UUID="92dc7073-bf4d-4c58-8052-63129ff5755b" TYPE="ext4"

controls@chiara|~> cat /etc/fstab

...

UUID=92dc7073-bf4d-4c58-8052-63129ff5755b   /media/40mBackup    ext4    defaults    0   0

Here I've used UUID rather than the device name "/dev/sde1" because the device name can get altered depending on the order of the usb connection.

This new disk is just a bare HDD drive sitting on the top of the chassis. We eventually want to accommodate this disk in the chassis so that we can recover the function only with the modification of /etc/fstab.  We need to wait for a next chance to have chiara down. In fact, when we can isolate chiara, we want to use this disk as the main disk and install another 4TB disk as a backup.

  14360   Fri Dec 14 22:19:22 2018 KojiUpdateGeneralChiara new USB 4TB DIsk

Edit: It was not 4TB disk but 6TB disk in fact. (We actually ordered 4TB disk...)

I think the problem of the backup disk was the flaky power supply for the external drive.
I swapped the drive to a new HGST 4TB one, but it was neither recognized nor spun up with the external power supply we had. So I decided to put both the new and old drives in the PC chassis to power them up with the internal power supply. I tested the old disk via a USB-SATA cable. However, this disk was not recognized. I noticed that the disk was not HGST 4TB but Seagate 3TB. Is it possible? I thought it was 4TB... Did I miss something?

Once the new 4TB was connected to the USB-SATA, it was very smooth to get it mounted. Now the disk is mounted as /media/40mBackup as before. /etc/fstab was also modified with the new UUID. All the command logs are found here below.

Let's see how the morning backup goes. It would take a while to copy everything on the new disk. So it was actually very nice to set this disk up by Friday midnight.


controls@chiara|~> lsblk

NAME   MAJ:MIN RM   SIZE RO TYPE MOUNTPOINT
sda      8:0    0 465.8G  0 disk 
---- sda1   8:1    0 446.9G  0 part /
---- sda2   8:2    0     1K  0 part 
---- sda5   8:5    0  18.9G  0 part [SWAP]
sdb      8:16   0   1.8T  0 disk 
---- sdb1   8:17   0   1.8T  0 part 
sdc      8:32   0   3.7T  0 disk 
---- sdc1   8:33   0   3.7T  0 part /home/cds
sr0     11:0    1  1024M  0 rom  
sdd      8:64   0   5.5T  0 disk 

controls@chiara|~> sudo mkfs -t ext4 /dev/sdd1

mke2fs 1.42 (29-Nov-2011)
Filesystem label=
OS type: Linux
Block size=4096 (log=2)
Fragment size=4096 (log=2)
Stride=0 blocks, Stripe width=0 blocks
183144448 inodes, 1465130385 blocks
73256519 blocks (5.00%) reserved for the super user
First data block=0
Maximum filesystem blocks=4294967296
44713 block groups
32768 blocks per group, 32768 fragments per group
4096 inodes per group
Superblock backups stored on blocks: 
    32768, 98304, 163840, 229376, 294912, 819200, 884736, 1605632, 2654208, 
    4096000, 7962624, 11239424, 20480000, 23887872, 71663616, 78675968, 
    102400000, 214990848, 512000000, 550731776, 644972544
Allocating group tables: done                            
Writing inode tables: done                            
Creating journal (32768 blocks): done
Writing superblocks and filesystem accounting information: done      

controls@chiara|~> blkid

/dev/sda1: UUID="972db769-4020-4b74-b943-9b868c26043a" TYPE="ext4" 
/dev/sda5: UUID="a3f5d977-72d7-47c9-a059-38633d16413e" TYPE="swap" 
/dev/sdc1: UUID="92dc7073-bf4d-4c58-8052-63129ff5755b" TYPE="ext4" 
/dev/sdd1: UUID="1843f813-872b-44ff-9a4e-38b77976e8dc" TYPE="ext4" 

controls@chiara|~> sudo emacs -nw /etc/fstab
controls@chiara|~> cat /etc/fstab

# /etc/fstab: static file system information.
#
# Use 'blkid -o value -s UUID' to print the universally unique identifier
# for a device; this may be used with UUID= as a more robust way to name
# devices that works even if disks are added and removed. See fstab(5).
#
# <file system> <mount point>   <type>  <options>       <dump>  <pass>
proc            /proc           proc    nodev,noexec,nosuid 0       0
# / was on /dev/sda1 during installation
UUID=972db769-4020-4b74-b943-9b868c26043a /               ext4    errors=remount-ro 0       1
# swap was on /dev/sda5 during installation
UUID=a3f5d977-72d7-47c9-a059-38633d16413e none            swap    sw              0       0
#UUID="90a5c98a-22fb-4685-9c17-77ed07a5e000"    /media/40mBackup       ext4      defaults,relatime,commit=60       0         0
UUID="1843f813-872b-44ff-9a4e-38b77976e8dc"    /media/40mBackup       ext4      defaults,relatime,commit=60       0         0

#fb:/frames      /frames nfs     ro,bg


UUID=92dc7073-bf4d-4c58-8052-63129ff5755b   /home/cds    ext4    defaults,relatime,commit=60    0   0

controls@chiara|~> sudo mount -a
controls@chiara|~> df

Filesystem      1K-blocks       Used  Available Use% Mounted on
/dev/sda1       461229088   10694700  427105320   3% /
udev             15915020         12   15915008   1% /dev
tmpfs             3185412        868    3184544   1% /run
none                 5120          0       5120   0% /run/lock
none             15927044        484   15926560   1% /run/shm
/dev/sdc1      3845709644 1809568856 1840789912  50% /home/cds
/dev/sdd1      5814346836     190408 5521130352   1% /media/40mBackup
  14361   Sat Dec 15 18:29:53 2018 KojiUpdateGeneralChiara new USB 4TB DIsk

The local backup was done at 18:18 after 11h18m of running.

2018-12-15 07:00:01,699 INFO       Updating backup image of /cvs/cds
2018-12-15 18:17:56,378 INFO       Backup rsync job ran successfully, transferred 5717707 files.

 

  10575   Tue Oct 7 10:09:07 2014 manasaUpdateGeneralChiara not responding

Chiara doesn't seem to be responding and I guess something happened 7 hrs ago.

I tried to hook up chiara to a monitor to reboot or atleast look for error messages; but it is not even detecting the external monitor (Tried changing monitors and vga cables; still see nothing).

I tried to ssh into it and only received errors :
NFS lookup failed for server XXX.XXX.XXX.XXX : error 5 (RPC: Timed out)
ssh: chiara: host/servname not known

Steve had the vacuum checked and everything seems fine with the status of the vacuum system atleast.

  10577   Tue Oct 7 16:19:50 2014 ericqUpdateGeneralChiara not responding

We're back! It was entirely my fault.

Some months ago I wrote a script that chiara calls every night, that rsyncs its hard drive to an external drive. With the power outage yesterday, the external drive didn't automatically mount, and thus chiara tried to rsync its disk to the mount point, which was at the time just a local folder, which made it go splat. 

I'm fixing the backup script to only run if the destination of the rsync job is not a local volume. 

  10578   Tue Oct 7 16:41:12 2014 JenneUpdateGeneralChiara not responding

I put a little script into ...../scripts/Admin that will check the fullness of Chiara's disk.  We only have the mailx program installed on Nodus, so for now it runs on Nodus and sends and email when the chiara disk that nodus mounts is more than 97% full.

  3438   Wed Aug 18 20:54:23 2010 rana, yoichiConfigurationEnvironmentChiller's chiller turned off

WE programmed the MOPA chiller's AC unit to turn off at 6PM each day and automatically turn on at 7 AM each morning. Its now very quiet in the control room at night.

Next, we'll leave it off during the day and see if it makes Steve go crazy or not.

  2096   Thu Oct 15 02:41:04 2009 ranaUpdateCOCChoice of folding mirrors in the RC cavities

In addition to the main mirrors (PRM, SRM) we will also have fold mirrors (called PR1, PR2, SR1, SR2). I am curious to see if we can get away with just using commercial optics; I think that the CVI Y1S coatings may do the trick.

Picture_9.png

The above plots show the reflectivities v. wavelength. I've asked the sales rep to give us specs on the reflectivity v. angle. I bet that we can guess what the answer will be from these plots.

  8966   Mon Aug 5 18:18:32 2013 gautamUpdateCDSChoosing LO Amplitudes and Frequencies

In order to decide what frequencies to dither the 4 degrees of freedom (M1-pitch&yaw, M2-pitch&yaw) at, I took the power spectrum of the X and Y-arm green transmission (C1:ALS-TRX_OUT, C1:ALS-TRY_OUT). Plots showing the power spectra are attached. Looking at the power spectra, I would think that for the X-arm, it would be okay to dither at 40, 50, 60 and 70 Hz. In order to check if the piezos could respond to these frequencies, I used my QPD setup and shook the PZTs with a 100Hz, 1Vpp sinusoid, and saw that the spot moved smoothly on the QPD.


 As for choosing the modulation amplitude, I did a simplistic approximation assuming that the misalignment only rotates the beam axis relative to the cavity axis, and determined what angle coupled 10% of the power into the next eigenmode. Assuming that this is small enough such that if we are already locked to TEM00, the dither won't kick it up to some higher-order mode, the LO amplitude should be in the range of 30-60 digital counts (determined using the PZT calibration constants determined here. This corresponds to a sine-wave of ~50mV amplitude reaching the PZTs (after HV amplification). I am not sure if this is too small, but according to the PZT datasheet, these platforms are supposed to have a resolution of 0.02 urad, which would correspond to the input signal changing by ~0.1 mV, so this signal should be capable of dithering the tip-tilt. 


 I have already added band-pass filters centered at these frequencies to the model (with a passband of 5Hz, 2Hz on either side), and low-pass filters to pull out the DC component of the output of the lock-in amplifiers. It remains to tune the gains of the filter stages. These parameters (frequency, amplitude of the LOs) may also have to be changed after tests). Hopefully the PZTs can be plugged in tomorrow, and I can try and make a measurement of the output matrix. 

Koji also suggested that it may be good to have a path in the model that feeds back to the PZTs by dithering the cavity mirrors as opposed to the PZT mounted mirrors. I will work on incorporating this into the SIMULINK model (c1asx.mdl) and also into the master medm screen.


 

Notes:

  1. The spot size of the X-arm green transmission on the PD was larger than the active surface. I moved the GTRX PD a little back and put in a lens (KPX085, 62.9mm FL, AR.14) in front of the PD, such that the spot is now occupying about 1/4th of the active surface area. The lens was mounted in a Thorlabs LMR1mount, and has been labelled.
  2. I made a slight change to the SIMULINK model, so as to calibrate the PZT sliders to (approximately) volts (I added a multiplier block that multiplies the slider value by constant value 3267.8). The idea is that we can approximately relate the slider value to tilt, knowing the calibration constant in mrad/V for the PZTs.

 

Power Spectra of Arm Green Transmission:

GTR_Power_Spectrum.pdf

  8968   Mon Aug 5 19:10:01 2013 KojiUpdateCDSChoosing LO Amplitudes and Frequencies

- I suppose the green transmission paths were thoroughly inspected and aligned in prior to the measurement

- Of course it is a BAD idea to use 60Hz as the LO frequency.

- Power spectra should be plotted as "RIN (relative intensity noise)" as the DC of 1 and 100 gives you 100 times different power spectra for the same beam.
  Don't forget to subtract the offset from your DC values.

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