TITLE: 02/14 Day Shift: 16:00-00:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Planned Engineering
INCOMING OPERATOR: None
SHIFT SUMMARY:
I covered first part of shift & handed over to Patrick as I assisted with HAM6 in-vac cable work. Main activities of the day so far:
LOG: (items in bold are ongoing)
Bubba G., Mark D., TJ
The install arm has been installed on the HAM6 South door for the OPOS (VOPO) install. Bubba and Mark started early to put the flange protectors on and hunt for hardware. I showed up just as they were lifting the arm into place. Both the arm and the HAM Structure Lift (D1001664) went on without any issues. I gave the arm a good cleaning and then put a cover on it and locked it into place. It should be ready for use next week.
Big thank you to Bubba and Mark!
TITLE: 02/14 Day Shift: 16:00-00:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Planned Engineering
OUTGOING OPERATOR: None
CURRENT ENVIRONMENT:
Wind: 5mph Gusts, 3mph 5min avg
Primary useism: 0.06 μm/s
Secondary useism: 0.23 μm/s
QUICK SUMMARY:
D Sigg, TVo
Cleaned up the naming conventions to make the heater library generic and added said library to PLC3 in the corner station. Re-scanned the system manager and linked the PLC variables to the terminals.
Sheila, Terry
We have swapped the input/output coupler on the H1 OPO. The original optic was M1 from E1600051, and we have swapped it now with E1700299, which has a reflectivity of 98% for 532, so that we can use our OPO as a reference cavity.
Although this optic is M1, the mount it is on is labeled M4 because the other M1 mounts were used already. We found that the optic was misaligned in pitch when we tried to swap it. We measured the distance between the prompt reflection about 10mm above the leakage beam at a distance of 500mm from the cavity (we are using the 1064 beam which was aligned into the input/output coupler for the escape efficiency measurement), meaning that the beam had a 1 degree misalignment or that the mirror was pitched by +0.5 degrees compared to the original optic.
We think the problem is the wedge of the optic. There is an arrow on the barel which is supposed to indicate the thick part of the optic, for the original M1 that arrow is on the side of the optic farther away from the crystal, so that the wedge is horizontal. For the new coupler, it is rotated about 45degrees clockwise from that position (the arrow is on the upper half of the barel, away from the crystal.) Since the wedge is a half a degree this probably explains the misalignment we see.
There is no way to adjust pitch in these mounts, but Hugh brought us some class A shims that were used for ISIs. Hugh suggested that we place the edge of the shim half way along the front feet on the mirror holder (D1600063), so that we would be able to adjust pitch by sliding it back and forth. We used a 5 thousandths of an inch shim and were easily able to adjust the optic pitch. The field used for the escape efficiency measurement is again aligned to the cavity.
Travis and Kissel spent the morning measuring violin modes of the new ETMY suspension (Kissel is digesting data). In the afternoon, Travis and I worked on aligning the reaction chain well enough that it would suspend without mechanical interference. We paused the round when we got the oplev main reflection beam (2nd beam up due to wedge of ETM16) on the oplev off center by under 100urad in pitch and yaw. We then realigned all of the top stage tablecloth brackets and install and aligned the top BOSEMs. After a few more rounds of iterative adjustment and alignment work, we repeated the process on the AOSEMs inside the PenRe mass. A few quick P and V TFs show that both the main and reaction chains are free, but will recheck tomorrow. Next up... mine for overnight spectra from tonight in order for Kissel to pre-tune the BRD assemblies that are due to be installed next.
Overall transmission: 95%
About 95% of the power going in is S-pol so the transmission was calculated based on everything that came out over S-pol power that went in. The half wave plate at the output of the isolator hasn't been fixed so it still spits out mostly P-pol. About .5% of what came out was S-pol (a half wave plate has been installed to fix the polarization).
Isolation: -30.5 dB
Usual set up: Mirror facing flat at the output and beam splitter at the input. I found a non-polarize beam splitter for 1064 this time. Assuming no losses in the reflection I measured the power that came back through the isolator and reflected off the beam splitter. Taken the known input power and the percentage of the reflected power before going into the isolator into account I calculated the total power that came back through the faraday.
J. Kissel, K. Kawabe I've taken L, P, and Y driven transfer functions of the final/bottom/optic/M3 stage of H1 SUS PRM to gather what the longitudinal-to-pitch cross coupling "typically" looks like for an HSTS. Also, I've compared the results against the HSTS dynamical model, just because I'd never focused on how poorly the off-diagonal elements of the model reproduce reality. Keita had asked me for the information to help validate the recent PRC spot position measurement LHO aLOG 40477. Attached are the results and the hacky, non-svn'd script used to generate it. #slapsownwrist Data lives here: /ligo/svncommon/SusSVN/sus/trunk/HSTS/H1/PRM/SAGM3/Data/ 2018-02-13_2350_H1SUSPRM_M3_WhiteNoise_L_0p01to50Hz.xml 2018-02-13_2350_H1SUSPRM_M3_WhiteNoise_P_0p01to50Hz.xml 2018-02-13_2350_H1SUSPRM_M3_WhiteNoise_Y_0p01to50Hz.xml
In the hope of making our lives simpler, I have created a wrapper bash script for svn commands. It checks the current working directory to determine which version of svn was used to create the directory, and then runs the appropriate version of svn client. It passes all the arguments given to itself onwards to the svn binary. The hope is that this is all totally transparent to the user.
The script is found in /ligo/cds/userscripts/svn which is a link to /opt/rtcds/userapps/release/cds/common/scripts/svn.bsh
If /ligo/cds/userscripts is ahead of /usr/bin in your PATH environment variable, you will be calling the wrapper script every time you run svn.
If you need to reconfigure your PATH to make this so, please add the following line to your .bashrc file in your home directory
export PATH=/ligo/cds/userscripts:/usr/bin:$PATH
you can confirm the path by typing 'which svn' which should return '/ligo/cds/userscripts/svn'
Now that the svn client version is tied to the working directory's version, you can find the version by running "svn --version"
For example, in /ligo/svncommon/SusSVN/sus/trunk/QUAD/H1/Common
svn, version 1.6.17 (r1128011)
whereas in /opt/rtcds/userapps/release/cds/common/scripts
svn, version 1.8.10 (r1615264)
A nice feature when checking out a brand new working directory is that, because there is no .svn directory, the script defaults to creating a 1.8 versioned working directory.
TITLE: 02/13 Day Shift: 16:00-00:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Planned Engineering
INCOMING OPERATOR: None
SHIFT SUMMARY:
LOG:
J. Kissel, T. Sadecki, B. Weaver Betsy and Travis are beginning to resurrect the top mass OSEMs on the newly re-suspended H1 SUS ETMY. In doing so, they've found R0 F2 OSEM's Test/Coil Enable BIO Frozen in OFF Position. Toggling the test/coil enable (TCE) state from 0 or 1 moves all of the rest of the R0 TCE switches, but F2's remains in the stuck position. This could be either the readback stuck, which wouldn't be a priority to fix, or it could actually be the switch that's dead, which would be a major blocker for activity. I attach a screenshot of the M0 / R0 corner of the binary IO screen showing the problem.
Opened corresponding FRS Ticket 9953.
This morning we looked at the electronics for the SUS test/coil enable readback for ETMY R0 F2 OSEM. Alog 40517 reports readback stuck in OFF state. We verified test/coil bit is switching inside the coil driver but the readback status change is not being captured by the binary card inside the IO chassis. Plan is to power cycle IO chassis. If error does not clear, binary card inside the IO chassis will need to be replaced.
F. Clara, R. McCarthy
Power cycle h1oaf0 in attempt to fix h1oaf overrun issue.
h1oaf0 was power cycled. The sequence was: kill models, take h1oaf0 out of the Dolphin fabric, power down cpu, power up cpu.
Note: no software was changed, no modified filter files were loaded.
The only restart issue was a brief IRIG-B negative excursion for h1iopoaf0, which invalidated the DAQ data and IPC channels for about 5 minutes.
Unfortunately, this does not fixed the h1oaf0 overrun problem (which started when h1ngn was decommissioned).
DAQ Restart
The DAQ restart was to:
use the latest H1EDCU_HEPIPUMPEX.ini
use a new H1EDCU_SEISMON.ini which I created from the new 6-eq_event code.
WP7346 Vacuum Alarms Reconfiguration
Chandra, Dave:
The cell phone alarm system was reconfigured to:
remove CP4 LN2 pump level alarms (value and error channels) from the system
increase CP4's vacuum gauge alarm level from 1.0e-07 to 5.0e-05 Torr.
The removal of CP4 LN2 pump data has impacted on the daily CP reports, which will require a code change later today.
2018_02_13 09:42 h1iopoaf0
2018_02_13 09:42 h1pemcs
2018_02_13 09:44 h1calcs
2018_02_13 09:44 h1iopoaf0
2018_02_13 09:44 h1oaf
2018_02_13 09:44 h1odcmaster
2018_02_13 09:44 h1pemcs
2018_02_13 09:44 h1susprocpi
2018_02_13 09:44 h1tcscs
2018_02_13 11:56 h1dc0
2018_02_13 11:56 h1nds1
2018_02_13 11:58 h1broadcast0
2018_02_13 11:58 h1fw0
2018_02_13 11:58 h1fw1
2018_02_13 11:58 h1fw2
2018_02_13 11:58 h1nds0
2018_02_13 11:58 h1tw1
This morning at 9:20am local I reduced CP4's LLCV setting to 0% open to cut off LN2 flow into pump reservoir. Kyle connected the HAM 6 backing cart with safety valve to CP4's turbo and will valve in turbo this morning before the pump warms up too much. Currently CP4 is at 58% full. Dave B. readjusted text/email alarms.
Mark D. is removing insulation from GN2 lines - sections that fall within bake inclosure.
Ken is removing electrical conduit, wiring, and supports and will continue this work throughout the week.
Kyle and Gerardo are stripping GV 11,12 of its wiring, controllers, annulus piping, etc.
I'm working with bake enclosure contractor on last minute "gotchas."
Rather than make Kyle work the graveyard shift, I've programmed the set point of CP4 to 20% full with some flow in the transfer line. Ideally we want the pump to dry out during the day when we're in 'work mode' to monitor the turbo-scroll throughput. Reservoir is currently 45% full. Linearally extrapolating yields ~5 hrs duration to fall from 20% to 0%.
The crew made excellent progress today stripping away external components.
We valved out the small ion pump connected to the bottom of CP4.
AIP is still pumping on GV12 due to leaky gate annulus and a pump cart is connected and running (valved out) in case of emergency.
CP4 will fall to 20% full at around 11 pm tonight (if linear) but will likely happen faster.
J. Kissel, T. Sadecki Travis and I used a HeNe Laser, QPD, and speaker array to begin characterizing H1SUSETMY's PUM-to-TST fused silica fiber violin modes. We were able to complete the characterization of 3 of the 4 fibers, but we began to have (we believe to be) electronics problems during characterization of the last fiber, so we've left the set turned off but otherwise as is, in hopes the the gremlins will go away by tomorrow morning to characterize the final fiber. I've exported the data, and intent to process it in detail as I've done for ITMX (see LHO aLOG 39163), but for now preliminary results are as follows (under the "Answer" column): Freq resolution 62.5mHz (400 lines with 25 Hz span) +X / +Y (S1400157; Partial Suspended Fundamental: 504.5 Hz) Freq Band / Hz Answer / Hz nAvgs Exc Amp / mV FileName 1st 490 515 504.8 10 250 0003 2nd 990 1015 999.8125 10 250 0004 3rd 1460 1485 1471.3125 10 250 0005 4th 1975 2000 1980 10 250 0006 5th 2450 2475 2460.3125 10 500 0007 6th 2925 2950 2939.625 10 500 0008 -X / +Y (S1400159; Partially Suspended Fundamental: 503.0 Hz) 1st 490 515 503.625 10 500 0009 2nd 990 1015 1000.3125 10 500 0010 3rd 1460 1485 1470.375 10 500 0011 4th 1975 2000 1979.4375 10 500 0012 5th 2450 2475 2459.4375 10 500 0013 6th 2925 2950 2939.375 10 500 0014 +X / -Y (S1800486; Partially Suspended Fundamental: 513.25 Hz) 1st 500 525 512.75 10 500 0015 2nd 1000 1025 1016.8125 10 500 0016 3rd 1490 1515 1500.375 10 500 0017 4th 1975 2000 1979.5625 10 500 0018 5th 2450 2475 2459.375 10 500 0019 6th 2925 2950 2939.3125 10 500 0020 So far, the difference between fully suspended and partially suspended values look consistent with the ~0.5 Hz shift down in frequency as seen on ITMX. Note, we tried upgrading the HeNe laser to a spare fiber-coupled optical lever laser as requested by Angus in LHO aLOG 40300, but the output coupler we were given collimated the beam to much larger than we needed (a ~10mm beam for a ~3mm QPD). Also, we were seeing a large amount of glitch-like impulses while taking the ASD of the QPD SUM output. A scope, time-series reading of the QPD output showed no glitching at any time scale. Suspecting the new laser, we tried out the old, supposedly noisy one. Simultaneously, I found that the SR785 input settings were DC coupled, and switched to A-B with AC coupling. Either the laser swap or the AC coupling fixed the problem, but since we were on a roll, we didn't switch back to the new spare optical lever laser. All of today's measurements were taken with the old HeNe laser.
I've fully processed the data, and I'm sad to say that this data set us much more poor than what we got for ITMX (LHO aLOG 39163). (1) With all of the electronics problems, and the lack of outside-world wifi at the end stations, we couldn't look at ITMX's results results during the measurement, and I ended up chasing features of the electronics above the 3rd harmonic. In other words, the frequencies of the ~2kHz and above modes are junk. Don't trust them. (2) We didn't spend the time to characterize the partially suspended violin mode fibers beyond the fundamental, so the comparison between partially suspended and fully suspended is not as complete. Attached are the same plots as before however, just for consistency. Below is the completed table -- to the best we can -- for the fully suspended, in-air violin mode measurements. Fiber S/N Harmonic Partially Fully df (F-P) +X / +Y S1400157 1st 504.5 504.81 +0.31 2nd No Data 999.81 n/a 3rd No Data 1471.31 n/a -X / +Y S1400159 1st 503.0 503.63 +0.63 2nd No Data 1000.19 n/a 3rd No Data 1470.38 n/a +X / -Y S1800486 1st 513.25 512.75 -0.50 2nd No Data 1016.75 n/a 3rd No Data 1500.31 n/a -X / -Y S1800491 1st 510.5 509.88 -0.63 2nd No Data 1008.69 n/a 3rd No Data 1492.31 n/a Please note I state in the above entry that "So far, the difference between fully suspended and partially suspended values look consistent with the ~0.5 Hz shift down in frequency as seen on ITMX." From the table in this entry, it is obvious this is incorrect, and some skew up and others skew down in frequency.
Patrick covered from 20:52 - 22:45. Activities for latter part of shift: