Displaying reports 63501-63520 of 77237.Go to page Start 3172 3173 3174 3175 3176 3177 3178 3179 3180 End
Reports until 11:40, Wednesday 24 September 2014
H1 PSL (PSL)
gabriele.vajente@LIGO.ORG - posted 11:40, Wednesday 24 September 2014 (14125)
Moving the beam on ISS using IM3

Sudarshan, Gabriele

Since yesterday we were not able to move the beam on the ISS QPD or PDs using the picomotors, today we tried to use IM3 to change the beam position. In brief, we are able to see a change in the QPD signal when we move IM3, so it seems there is a beam on the QPD. We read a sum of about 830 count on the QPD, which corresponds to 0.5 V. The transimpedance should be 100kOhm, so the power on the QPS should be of the order of few microwatts, while we expect 1% of the total power going into the ISS box, which should be more like 0.1 mW.

We couldn't see any change in the mean value of the PD signals, however the RMS could be changed a lot, see the striptool trace. The initial position of IM3 was: PIT 55500, YAW 2600. The one corresponding to the largest RMS in the PDs was PIT 59500, YAW 1600.

The second plot shows a comparison of the PD spectrum (dewhitened) in the original position (red) and in the new position (blue). There is significantly more signal in the new position.

In summary

  1. If we move the beam into the ISS box we can change the level of signals on the PDs
  2. There still seems to be too low power, even on the QPD
  3. We were not able to move the beam using the (old) picomotor, so this is likely not working
Images attached to this report
H1 TCS (TCS)
aidan.brooks@LIGO.ORG - posted 10:47, Wednesday 24 September 2014 (14123)
ALS green leakage makes it to HWS table

Aidan. Greg.

We removed the yellow viewport covers on HAM4 by the Hartmann sensor table (the acrylic covers are still in place). As expected, there was a leakage of the green ALS-X beam coming out of the HWSX and HWSY viewports (the HWSY green beam comes from the reflection of the ALS-X beam from the 50/50 surface of the beamsplitter, the HWSX green beam from the reflection of the ALS-X beam from the AR surface of the BS). The beams are incident on the apertures in the HWS table.

The beams are not centered on the apertures. However, due to the proximity of the HWS table to the H1-TCS-R1 rack (there's about 3"  and a lot of cables between them), and due to adequate clearance of the green beams (~2") from the edge of the apertures, I elected not to move the table any closer to the rack to center the beams more than they already are.

HWSX:

 

HWSY:

Images attached to this report
H1 CDS (SEI)
james.batch@LIGO.ORG - posted 09:43, Wednesday 24 September 2014 (14122)
Rebooted h1seib2
The I/O chassis of h1seib2 died Tuesday evening, requiring a power cycle of the I/O chassis and h1seib2 computer.
H1 SUS (ISC)
kiwamu.izumi@LIGO.ORG - posted 09:10, Wednesday 24 September 2014 (14121)
MC2 suspension restored

The MC2 suspension have been misaligned by the guardian since 8:00 pm last night probably for the green light activity. I restored it at 9 am this morning.

LHO VE
john.worden@LIGO.ORG - posted 08:28, Wednesday 24 September 2014 (14120)
Vacuum System open to the arms

We  opened to both arms yesterday. The attached shows the result of exposing the chambers to the 80K pumps and the arms.

Images attached to this report
H1 CDS (DAQ)
david.barker@LIGO.ORG - posted 07:37, Wednesday 24 September 2014 (14119)
CDS model and DAQ restart report, Tuesday 23rd September 2014

model restarts logged for Tue 23/Sep/2014
2014_09_23 02:28 h1fw1
2014_09_23 11:49 h1ascimc
2014_09_23 12:46 h1ascimc
2014_09_23 12:59 h1ascimc

2014_09_23 16:06 h1broadcast0
2014_09_23 16:06 h1dc0
2014_09_23 16:06 h1fw1
2014_09_23 16:06 h1nds0
2014_09_23 16:06 h1nds1
2014_09_23 16:07 h1fw0

unexpected restart of h1fw1. ASC-IMC model work with associated DAQ restart.

H1 CDS (SEI)
david.barker@LIGO.ORG - posted 07:14, Wednesday 24 September 2014 (14118)
h1seib2 front end down

all the models on h1seib2 (Seismic Beam Splitter) stopped running around 7pm Tuesday night PDT. Looks like the IO Chassis is having problems.

H1 ISC
sheila.dwyer@LIGO.ORG - posted 22:39, Tuesday 23 September 2014 (14117)
X arm locked with green

Alexa, Keita, Gabrielle, Dan, Sheila

The bottom line: X arm is locked on green, we are having trouble finding the beam on ITMY and it might be helpfull to have a camera on ITMY tomorow. 

Both PLLs are now working.  Both beatnotes needed to be realinged.  I reduced the power on the end Y BBPD, and realinged the laser green power monitor diode which was totally off. 

We spent some time searching for the green beam on the ITMY baffle PDs, but didn't find the real beam, I think. 

There is a beam which doesn't seem to have enough power, which can be found on PD1 at 2.2PIT, 7.3 YAW (20dB gain setting we get 3.6 Volts)  PD4 at -97.8 PIT 74 YAW (3.6 Volts, 20dB setting) When aligned to the center of these points, there is no beam arriving on ISCT1, and we could not find any return beam on the ETM baffle PDs even after a long search.  The ETM baffle PDs are working, since they clearly see the IR when PRMI flashes.  I have left  slow excitations on TMSY pitch and YAW hopping that at some point we will see light on the ITMY baffle PDs. 

Other things today:

Keita and I briefly tried to move the bem spot on PR2, using the output matrix he described here :  alog 13939

To do this we coped the gains from the opticalign filter banks into cal filters for pitch and yaw of iM4, PRM, PR2, and PR3.  However, when I briefly tried moving the spot around I misaligned the cavity. 

Gabrielle and I also tried locking DRMI using the configuration Kiwamu described from last night.  We were able to see any lock longer than a few seconds. 

PRMI however seems to be locking consistenly within a minute. 

Images attached to this report
H1 SEI
hugh.radkins@LIGO.ORG - posted 18:14, Tuesday 23 September 2014 (14114)
WHAM6 HEPI TFs set to start 2310 tonight running on opsws1

Thanks-H

H1 PSL (PSL)
gabriele.vajente@LIGO.ORG - posted 17:20, Tuesday 23 September 2014 (14110)
ISS work summary

Sudarshan, Peter, Keita, Gabriele

Checking the power on the diodes

According to the electornic schematics, the ISS second loop transimpedance board has two parts:

With the present input power of 10 W, we should have something like 10 mW into the array, which means 1.25 mW per photodiodes, corresponding to about 1.0 mA of photocurrent. After the transimpedance we should get 1.6 V  and 160 mV at the output of the board. This should corresponds to about 260 counts. However, we see that the RMS of the photodiode signals is about 17 counts and dominated by high frequency, while the mean value is ver close to zero, about 1 count (see second attachment, one minutes of data). It seems that we're not getting all the power we should.

We also checked in the electronics lab, with one spare board, that sending 1 mA at the input gives the expected signal levels both after the transimpedance stage and at the output. We also checked that adding a long cable at the input doesn't have any effect on the result.

Calibration of PD signals

Using the nominal whitening transfer function and transimpedance, we computed the calibration filters t be implemented in the PD filter banks. We don't want to have any 10 mHz pole, so we actaully fitted the whitening ransfer function between 1 Hz and few kHz, see third attachment (blue nominal TF, green implemented TF). Therefore, the PD_OUT signals are calibrated in mA only between about 1 Hz and 5 kHz. Below and above the signals are uncalibrated. This is expecially true for the DC level, which is not correct. Later on, once we'll have solved the missing power problem, we'll implement a calibration in units of RIN.

The result are shown in the forth attachment. The high frequency content of the 1-4 diodes (one board) is clearly different from the 5-8 diodes (the other board). We still don't know if this is due toa really different signal or to a different response of the board. Again, once we'll have solved the missing power problem, we'll see if this difference is still there.

Picomotor game

Right now we are quite sure that the beam is not properly hitting the PDs:

  1. the power level is very low
  2. the signal level on the eight diodes is quite different
  3. there is a large coupling of angular motions to power

So we wanted to move the beam using the two mirrors with picomotors. Of them, we were sure of the cabling of only the older one, which is the one closer to the ISS box and after the telescope. To make the story brief, we moved the picomotor by few 10000 steps in horizontal, bua saw no difference either in the QPD or PD signals. We could however see some "shaking" of the signals. Instead, moving in the vertical direction produced no result. So we're not sure if the picomotor is actually working. As for the second picomotor, we could not understand if it's cabled or not.

More investigations on the pico story tomorrow...

Images attached to this report
Non-image files attached to this report
H1 PSL
patrick.thomas@LIGO.ORG - posted 16:58, Tuesday 23 September 2014 (14111)
PSL chiller maintenance
The water level is near the max line and does not appear to need to be filled.
LHO General
patrick.thomas@LIGO.ORG - posted 16:52, Tuesday 23 September 2014 (14109)
Ops Summary
07:56 Hugh running transfer functions on HAM6
08:33 Aidan to HAM4 to connect electronics for Hartmann sensor
08:37 Portable toilet service
08:41 Alexa to end Y to check layout of ISCT table
08:45 Filiberto and Manny pulling cables for TCS near HAM4
08:46 Bubba craning 3IFO equipment at mid X (WP 4862)
09:03 Danny S. to LVEA test stand
09:29 Hugh to HAM6
09:45 Unifirst delivery
09:54 Alexa back from end Y
09:59 Hugh back from HAM6
10:17 Kyle starting work to open beam tube arms (WP 4863)
10:18 Alarm on LT150 cyropump (delivery?)
10:43 Kiwamu compiling and restarting the H1ASCIMC model (WP 4864)
11:46 Kiwamu restarting H1ASCIMC model
12:06 Chris to clean at mid X after lunch
12:44 Kiwamu restarting H1ASCIMC model
12:55 Danny S. to LVEA test stand
12:57 Kiwamu restarting H1ASCIMC model
13:17 Sheila to end Y to lock ALS laser to PSL
13:24 Aidan back to HAM4
~15:20 Fire department on site to check trouble alarm
15:40 Betsy to LVEA test stand
15:44 Peter, Keita to look at electronics racks near HAM2
16:05 Jim B. restarted the DAQ for the H1ASCIMC model change

High dust counts in the Vacuum Prep Lab
H1 TCS (TCS)
aidan.brooks@LIGO.ORG - posted 16:32, Tuesday 23 September 2014 (14108)
H1-TCS-R1. HWS computers see cameras.

Aidan. Greg.

Filiberto helped dress the cables in the H1-TCS-R1 rack. All the connections to the HWS table are now secure. I was able to turn on the HWS cameras and RCX C-Link converters remotely with the Beckhoff system. And I was able to log into H1HWSMSR and successfully connect to the HWS cameras.

HWSY

> serial_cmd -c 0

>> gcp

returns camera information

HWSX

> serial_cmd -c 1

>> gcp

also returns camera information

LHO General
patrick.thomas@LIGO.ORG - posted 16:11, Tuesday 23 September 2014 (14104)
periodic high dust counts in the LVEA
It appears that around noon each day, including on weekends, both the dust monitor in the beer garden and near HAM 6 are registering high dust counts. A plot of minute trends for the last 30 days is attached. Location 15 is in the beer garden. Location 6 is near HAM 6.

It started near HAM 6 on Sept. 4 and in the beer garden around Aug. 30.
Non-image files attached to this report
H1 DAQ (CDS)
james.batch@LIGO.ORG - posted 16:09, Tuesday 23 September 2014 (14105)
Restart data concentrator
Restarted data concentrator (and frame writers, nds, and broadcaster) to clear the bad DAQ status on the h1ascimc model.
H1 SEI (DetChar)
jeffrey.kissel@LIGO.ORG - posted 15:09, Tuesday 23 September 2014 - last comment - 22:32, Tuesday 23 September 2014(14099)
HAM2 ISI Single Saturation WD Trip
J. Kissel, J. Warner, K. Izumi.

Jim and I were working on ETMX; wiamu rolled over asking us what's up with HAM2 ISI. It had single-saturation tripped on actuators. We've got no idea. Our best guess is Kyle jumping around opening up the ARMs, but it's a terrible guess and probably not right. Sensor correction on HAM2 has been turned off since this morning.

#fortherecord
Images attached to this report
Comments related to this report
sheila.dwyer@LIGO.ORG - 22:32, Tuesday 23 September 2014 (14115)

HAM 2 tripped again later.

H1 SUS
betsy.weaver@LIGO.ORG - posted 10:58, Tuesday 23 September 2014 - last comment - 19:32, Tuesday 30 September 2014(14095)
3IFO QUAD 06 Phase 1B testing

QUAD 06 (Q6) Phase 1B transfer function plots are attached.   We had a hard time obtaining good coherence in the Transverse TF, so it is a bit hashy.  Will try again.  

 

Most notably is that, like Q8, the second pitch mode frequency is unexpectedly pushed upward on the main chain.  Recall, we never found the mechanism to fix it on Q8.  Interestingly, both the Q8 and Q6 assemblies are of the same batch of wires and are fresh builds, but by 2 different assembly teams, and on 2 different solid stack/test stand units.  Q8 is an ETM type of QUAD while Q6 is an ITM QUAD, but both main chains have the same pendulum parameters - both are detailed in the 'wireloop' model.

 

The Q6 data is plotted as QUADTST.

Non-image files attached to this report
Comments related to this report
betsy.weaver@LIGO.ORG - 15:14, Tuesday 23 September 2014 (14100)

We've checked that all wire diameters are as per the specs and that the wire segment clamps are seated properly on the masses.  We've also checked that the wire segments have been assembled with the proper assymetry as per specs (looking for something obvious).

 

Attached are pix of this unit, in case someone wants to look at them.  To me, they look just like the last few QUADs we've built, including Q8.

Images attached to this comment
brett.shapiro@LIGO.ORG - 17:20, Tuesday 23 September 2014 (14112)

Maybe this is a long shot, but we've exhausted all the simple causes...could the top wire be the wrong material? If the modulus of elasticity was higher, within a factor of 2 from where it is supposed to be, that would explain this strange pitch mode.

One way to test this is to measure the violin modes of the topmost wire in situ and see if it is right. Or maybe more simply, cut some wire from this wire stock, hang some wieght off of it, and measure its violin mode.

The correct 1.1 mm diameter wire should have a violin mode of 

frequency in Hz = sqrt(tension/0.0067)/(2*L)

where 0.0067 is the mass per unit length.

 

For example tungsten has a modulus about 2 times higher than what we are supposed to have. If for whatever reason we ended up with a tungsten wire, it would have an in-situ violin mode in the low 200s of Hz, rather than the 332 Hz spec (much denser than the usual piano wire).

brett.shapiro@LIGO.ORG - 17:52, Tuesday 23 September 2014 (14113)

Or even more simply, you could weigh some length of wire. The piano wire should be something close to 7 g/m. If you get different value from that, then the wire is the wrong material.

betsy.weaver@LIGO.ORG - 15:52, Wednesday 24 September 2014 (14129)

To confirm Brett's latest suggest regarding the wrong wire:  We have 2 rolls of 1.1mm diameter top wire here at LHO which could have possibly been used for QUAD builds.  Both are labeled as the correct stuff.  We weighed a 1m segment from each spool.  One measures 7.1g, the other measures 7.3g.

 

To be continued...

betsy.weaver@LIGO.ORG - 15:59, Wednesday 24 September 2014 (14131)

Another sanity check:

The Top Mass blade sets used for these 3 pitch-problematic QUADs are as follows:

Q6 - SET 10

Q8 - SET 8 - although I can't find the actual records

Q9 - SET 2

 

Q7 - SET 7 - still to be tested, unknown pitch frequency TFs

 

The SETs go from SET 1 being the most STIFF to SET 16 being the most SOFT.  So, the sets we are using for the 3IFO QUADs are somewhat scattered or in the middle of the pack.  They are not all clustered at the soft end, nor all at the stiff end...

betsy.weaver@LIGO.ORG - 14:43, Thursday 25 September 2014 (14151)

And here's the spectra of this Q6.  Note, the lowest stage (L2) does not have flags during the all-metal Phase 1 assembly, so the spectra plots of L2 are junk.

Non-image files attached to this comment
betsy.weaver@LIGO.ORG - 16:16, Thursday 25 September 2014 (14155)

And now attached are a damped TF from each R0 and M0.  As we all have noted in SUS - damped TFs on Phase 1 test stands are not useful since the damping is a function of the code on the out-dated test stands and the loops are not tuned very well.  Long story short, there is a little bit of damping evident, given whatever filters and gains are loaded, and we can see healthy excitations run through the suspension so all seems well with damping capabilities of Q6.

Non-image files attached to this comment
brett.shapiro@LIGO.ORG - 19:32, Tuesday 30 September 2014 (14235)
I ran the matlab model fitting code on the wireloop model for QUAD06. I used the measured top mass resonance frequencies, as well as the long-pitch frequencies from the triple hang data that Betsy collected. The latter was extremely helpful in refining the results beyond what top mass TFs provide on their own.
 
NOTABLE RESULTS:
 
* The top mass and UIM inertias converged to the same values obtained from the fiber H1ETMY fitting results (lho log 10089), within the error bars. This includes +12% on the UIM pitch inertia from what is given in the final quad design doc T1000286. Note, this means the same large shift has been found on two different configurations of different quads. So it is likely that the fitted value is correct. But great news for consistency on the suspensions.
 
* Some of the d's moved significantly. However, the move is noticebly less if you start from the previous fit to H1ETMY rather than the base model.
    -dn (top blade tip) increased by 1.25 mm relative to the H1ETMY fit. It is +2 mm relative to the base model. Note, one could alternatively shift dm instead.
    -d1 (uim blade tip) did not move significantly relative to the H1ETMY fit. However, it is +3 mm from the base model. Note, one could alternatively shift d0 instead.
    -d2 (PUM round prism, not part of fiber model) decreases by 1.25 mm.  This actuall could be due to errors in my previous estimate of what this value should be. In fact, this shift puts it about where it is supposed to be for the fiber quad.          Not sure if that is the intent with this prism.
 
* Still not clear what caused the shift in dn (or dm) relative to previous suspensions, like H1ETMY. The model fitting wouldn't say that though. All it can do is say that either dn or dm is off.
 
 
MORE DETAILS:
 
Plots of comparisons of the before/after models against the meadured data are attached. The first 6 pages show the top mass TFs. The 7th and final page merely shows the triple hang long-pitch frequencies since this data was pulled from an amplitude spectrum. In these plots, there are notable shifts in just 2 modes. The 2nd pitch mode (1.5ish Hz) on the top mass TF, and the first mode of the triple hang (0.4ish Hz), which is also pitch. The updated model shows pretty good agreement all around.
 
The parameter shifts required to make the match were originally rather large, for both the d's and the pitch moments of inertia. Interstingly, the moments of inertia for all the top two masses (didn't need to float the lower ones) consistently converged to the model fitting results from the fiber ETMY quad. Thus, I updated the wireloop model (update not committed to the svn yet) with the fitting results from H1ETMY for all the parameters of the top two masses (springs, inertias, d's). I then used this updated wireloop model as the staring point for the model fit.
 
The shifts in the parameters are below. The d's moved noticeably. The spring stiffnesses did not move a great deal, but were useful in fine-tuning the fit. The inertias did not need any further refinement from H1ETMY. I find this last point extremely exciting.
 
* mm shifts in the d's from H1ETMY fitting results
dn: 1.2438 +- 0.069243 mm   -> top mass blade spring tip
d1: 0.38916 +- 0.16088 mm   -> UIM blade spring tip
d2: -1.2815 +- 0.10267 mm    -> round PUM prism
 
* % shifts in the blade spring stiffnesses from H1ETMY fitting results
kcn: 2.1235 +- 1.8491 %         -> top-most blade stiffness
kc1: 0.56079 +- 0.45919 %     -> top-mass blade stiffness
kc2: -1.493 +- 0.58382 %        -> UIM blade stiffness
Non-image files attached to this comment
H1 ISC
sheila.dwyer@LIGO.ORG - posted 22:39, Monday 22 September 2014 - last comment - 22:34, Tuesday 23 September 2014(14088)
PRMI on 3F, evening seismic

Alexa, Gabrielle, Kiwamu, Sheila

This morning we moved PRMI to the 3F sensors, we used a gain of 3 in the input matrix to move PRCL from REFL 9 I to REFL 27 I, and a gain of 15 to move MICH from REFL 45 Q to REFL 135 Q.  This was locked from about 22:26:55 UTC (september 22) to 22:33:20. 

We then tried to move on to DRMI but have struggled most of the day to get it locked.  We locked it a few times this morning, (21:00 UTC) but haven't been able to recently. 

Also, as is typical recently, the anthropogenic noise is higer durring the evenings than durring the day, there must be an evening shift of hanford work.  Screen shot of the last week is attached. This pattern started in mid august and has been true since then.

Images attached to this report
Comments related to this report
kiwamu.izumi@LIGO.ORG - 01:06, Tuesday 23 September 2014 (14089)

After Sheila left, Jeff and I saw the DRMI locked for a minute or so at around 6:06 UTC. However, after this lock, the DRMI never caught a fringe again.

The settings at that point were:

  • MICH gain = 0.5
  • PRCL gain = 2.8
  • SRCL gain = -20

Also, I experimentally had an off diagonal element of -1 in the REFL_A_RF9_I to SRCL element together with the usual REFL_A_RF45_I to SRCL element at that point. Since there was a 3 Hz oscillation in MICH when it was locked, I increased the MICH gain by a factor of three, but this did not help at all.

sebastien.biscans@LIGO.ORG - 16:22, Tuesday 23 September 2014 (14107)

I did a quick comparison between the 'evening' (high BLRMS between 1 and 3 Hz as Sheila mentioned) and the 'night' (quiet time).

By looking at the ground, we do see some amplification in the spectrum around ~2.5Hz by almost a factor of 10. However, there is not a lot of power at those frequencies and this amplification doesn't seem to affect the optical lever motion (I looked at PR3).

I'll do a further analysis tomorrow and see what SUS and SEI are doing, but I wouldn't bet this is your issue so far.

Images attached to this comment
sheila.dwyer@LIGO.ORG - 22:34, Tuesday 23 September 2014 (14116)

I also don't think this is the reason we have not been locking DRMI, since th situation was similar on the nights we did lock, and the fringe speed is 1-2 fringes per second.  It is just interesting that we are actually louder at night than durring the day.

Displaying reports 63501-63520 of 77237.Go to page Start 3172 3173 3174 3175 3176 3177 3178 3179 3180 End