I selected a loud sine-gaussian injection done during ER7 at each site and compared h(t) data from the HOFT frames against the intended strain waveform; this is documented at https://wiki.ligo.org/Main/HWInjER7#Injection_sign_check . It looks like the injection came through with the wrong sign at LHO, but with the right sign at LLO. This should be investigated.
(evan jenne nic)
We wanted to investigate the OMC alignment/backscatter problem. Driving the OMC SUS in Yaw has been known to cause backscatter noise due to the modulation of the optical path length when the OMC moves in Yaw.
Our procedure was to lock the vertex optics in a bright michelson configuration (a state has been added to the IFO_ALIGN guardian to make this easy). Then we wanted to drive the OMC in yaw and choose the yaw->longitudinal matrix element such that the center of rotation would be about the input beam, rather than the omc center of mass. This would be determined by minimizing the scatter as measured by either OMC trans, or the MICH error point.
I was surprised that we were not able to induce any significant backscatter fringe wrapping noise in this configuration. We drove the OMC SUS in longitude up to the point that the beam was misaligning enough to noticibly affect the OMC DC trans.
We also drove the ISI table directly by putting a 1Hz 1mm injection into the Y isolation loop error point.
Driving the path length, we both listened and had a live spectrum running. We saw no evidence of scatter in either OMC trans or MICH_IN1.
We will need to think if there is another configuration (available to use without arms) that will be more sensitive to backscatter.
I forgot to mention that we turned on the AS fast shutter and OMC pzt high voltage supplies for HAM6.
This measurement didn't work because I was wrong about the calibration. The isolation loop error points are in nanometers, not micrometers. So we were moving the table 1000 times less than I thought.
8:52 Sudarshan work on ISS
Fil to EX (run cables)
9:16 Jordan to HAM6 checking on PEM sensors
9:44 Kyle to HAM6
10:01 Kyle grab He bottle at EY
10:15 Leo - EX ESD measurement
10:20 Kyle out of EY
11:25 Dave and Stefan to EY - Hook up GPS receiver
11:32 Fil & Andrea back from EY
11:50 Jordan to LVEA testing PEM accelerometer
12:04 Leo done with EX ESD measurement. Starting EY ESD measurement.
12:47 Jordan back
13:00 Kyle to EX
12:42 ISI HAM5 tripped
-No correlation with PEM acc. sensors. Not sure what happened. Coincides with sharp peak on 1-3 Hz ground motion plot. Suspect electronics issue.
13:42 Fil and Stefan to EX by the rack
13:53 Jordan to EX
14:12 Leo finished EY ESD measurement
14:24 Rick and Sudarshan to LVEA - ISS work by PSL enc.
Kyle back
14:37 Jordan to EY
15:00 Fil & Stefan back
15:10 Rick & Sudarshan back
15:19 Sudarshan & Jordan to IOT2R table
15:27 Kyle to HAM6
15:41 Kyle back. Shutdown HAM5, HAM6 annulus pump.
Other notes:
- Jordan discovered magnetometer at EY rack output straight line since June 22nd.
- Laser Hazard notifications added to Ops Overview.
HAPPY HOLIDAY!!!!
More charge measurements. Plots are attached.
Jim, Daniel
I calibrated the frequency of the CsIII Cesium Standard Atomic Clock in MSR by setting the Output Frequency on to 1 + (1010 * 10^-15). I did this at 12:26 PDT on July 2, 2015. I used the serial port on the back of the clock and the Monitor2 software installed on the IBM Thinkpad in MSR.
The previous setting was +1078 (parts per 10^15); I calculated the proper value to be 1010 (details below). I used the time difference between the atomic clock's 1PPS signals and our timing system's 1PPS signals. I took a linear regression to determine the rate of linear drift of the CsIII, since an improperly calibrated Cesium clock shows very little short-term jitter but does show long-term linear drift. Our timing system is long-term accurate since it's GPS backed.
I interpreted the meaning of the time difference according to an explanation from Daniel: a negative time difference means that the external (i.e. Cesium) 1PPS signal is ahead, while a positive time difference means it's behind. I calculated the drift rate to be approximately -6.8e-14 corresponding to -175 ns per 30-days.; the CsIII 1PPS is getting earlier and earlier relative to the timing system 1PPS, suggesting that the period is a bit short. I calculated the proper setting for the CsIII, as explained below, and talked to Microsemi's customer support to confirm that the CsIII's output frequency setting is what one would expect (the instructions were vague). He agreed with my interpretation but didn't have deep knowledge of the system. So we'll have to keep an eye out and check the drift rate in a few weeks to see if it is indeed close to zero (I expect it
will be fine).
The offset to be entered was calculated as follows. The current 1PPS period is given by tau_{measured} - 1 = m_{drift} where m_{drift} is the drift rate. If the clock's "natural" frequency is f_{natural}, then the current offset (Delta{f})_{measured} (which I found to be 1078 * 10^{-15} according to the Monitor2 interface) relates to the current measured period as (1 + (Delta{f})_{measured})f_{natural} = f_{measured} = frac{1}{tau_{measured}}. We want f_{calibrated} = 1, so we need to set (1 + (Delta{f})_{calibrated})f_{natural} = 1 = (1 + (Delta{f})_{measured})f_{natural}tau_{measured}, which simplifies to 1 + (Delta{f})_{calibrated} = (1 + (Delta{f})_{measured})tau_{measured}, giving (Delta{f})_{calibrated} = (1 + (Delta{f})_{measured})tau_{measured} - 1 = (tau_{measured} - 1) + (Delta{f})_{measured}tau_{measured}, or, in terms of the drift rate, (Delta{f})_{calibrated} = m_{drift} + (Delta{f})_{measured}(1 + m_{drift}), which we then divide by 10^{-15} in order to get the value to be entered into the Monitor2 software. See the attached code (written in Julia) for the precise method used. The output (besides the graphs, also attached) includes the above calculations:
Drift rate in Time Code Generator in MSR: -6.786047272268983e-14
Drift rate in Time Code Translator in EX: -6.788794482601771e-14
Drift rate in Time Code Translator in EY: -6.780539996010063e-14
mean_drift_rate = mean($(Expr(:comprehension, :(channel.drift_rate), :(channel = channels)))) => -6.785127250293606e-14
delta_f_measured = 1.078e-12 => 1.078e-12
delta_f_calibrated = mean_drift_rate + delta_f_measured * (1 + mean_drift_rate) => 1.0101487274969909e-12
what_to_enter_into_monitor2 = delta_f_calibrated / 1.0e-15 => 1010.1487274969908
Note that the drift rates calculated for each channel are in very close agreement. I used this to pick the new setting of 1010 for the Cesium clock. The channels I looked at were:
H1:SYS-TIMING_C_MA_A_PORT_2_SLAVE_CFC_TIMEDIFF_1 (Time Code Generator in MSR)
H1:SYS-TIMING_X_FO_A_PORT_9_SLAVE_CFC_TIMEDIFF_1 (Time Code Translator in EX)
H1:SYS-TIMING_Y_FO_A_PORT_9_SLAVE_CFC_TIMEDIFF_1 (Time Code Translator in EY)
The timeseries (with linear regressions) and histograms are included. The period analyzed is from the beginning of ER7 until last week. I had to remove a chunk of spurious data from the EY channel since Dave and I were using the BNC cable for a different test and polluted the EY channel during that time.
The linear regression shows a very clear and steady trend, as expected. Standard deviation of the atomic clock offset is reduced by a factor of five once linear drift is accounted for, and the histogram more closely follows a Gaussian distribution:
std(z) => 1.1845358220722136e-8 # Jitter about linear trend
std(y) => 5.853090568967089e-8 # Absolute time difference
Filiberto, Jim, Dave Installed one new CNS Clock II in each end station in receiving, directly above the Timing IRIG-B Module in each rack. We tested each unit to make sure it successfully locks to a GPS signal. Filiberto ran an extension cable for the GPS antenna from VEA into receiving in both end stations in order to provide signal for the new CNS II as well as a BNC cable from receiving to CER to deliver the CNS II 1PPS signal to the third time difference port of the Timing Comparator located there. The cable lengths for the 1PPS signals are the same to within an inch.
Upon completing the leak testing of the Y-end yesterday, Gerardo and I realized that we had failed to test the 4.5" blank which had replaced the 1st generation ESD gauge on BSC9 at the X-end. So... ~1345 - 1415 hrs. local Replaced X-end turbo scroll baking pump with LD and sprayed 20 seconds of audible helium flow at untested CFF -> OK -> Restored pump configuration to as found -> Shut down LD
Scott L. Ed P. 6/30/15 Cleaned 62 meters ending 1.5 meters north of HNW-4-097. 7/1/15 Cleaned 47.4 meters ending 13 meters north of HNW-4-099. 7/2/15 Finished crevice cleaning and testing. Results posted here. X-ARM IS COMPLETE.
This is the (delayed due to conference travel) summary of my DQ shift for 12-15 June mentored by Andy L, the detailed report is at https://wiki.ligo.org/viewauth/DetChar/DataQuality/DQShiftLHO20150612
Several blip glitches occurred during that time, eg this one
DAC glitches were noticed in LSC-MCL_IN1, these seem to come from SUS-MC2_M3 as shown by the lineup plot :

Much of the data was clean with good sensitivity - but there were significant bad periods of excess broadband and/or low frequency noise during hour 8 UTC (spectrogram link) and hour 10 UTC (link) which killed inspiral range. The excess noise appears also in a large number of ASC and LSC channels but no clear cause. Does anyone have an idea what could have been going on at these times?
One curious feature was a band of excess noise over 60-75 Hz appearing at almost exactly 12:00 and gradually moving up and down in frequency until hour 17 UTC when it suddenly disappeared. See spectrogram link for an overview. Again this is mysterious and any clues from on side would be welcome.
It is clear from the spectrograms and omicron triggers that there were a few (about 1 per hour) really loud glitches - SNR > 1000. It has been suggested these are related to beam tube cleaning and its aftermath (e.g. particles loosened & falling through the beam). See omega scan of the loudest
Another feature seen previously is a set of near-periodic glitches at 60Hz, approximately every 72 minutes. These are associated with activity in the SUS-ETMY_L2 auxiliary channel, 'something happening' at the Y arm end station with ~4300s period.
Forgot to post this yesterday. This is the Ops Summary for Wednesday July 1st.
8:26 Leo - ETM ESD charge measurement
8:56 Jodi/Jeff to warehouse and Mid Y
9:22 Elli to IOT2R
9:30 Jodi and Jeff B. back
9:35 Gerardo to EX, EY pick up equipment
9:36 Elli to EY
9:41 Jordan to EX testing PEM acc. meter.
10:01 Elli back
10:10 Karen to LVEA
10:17 Jeff K. to LVEA (ISC rack by PSL room)
10:40 Jeff K. back
10:41 Jeff B. to 3IFO area
10:58 Ed to ETMX increase oplev laser power
11:03 Jeff B. back
11:12 Gerardo back
11:14 Fil to End stations - run cables for second pressure gauge
11:22 Gerardo back
11:50 Jason, Ed test turning off HPO box
12:00 Jason, Ed back
12:16 Fil back
13:01 Jordan back
13:07 Kyle climbing on HAM6
13:34 Kyle - vacuum work around HAM6
13:50 Gerardo climbing HAM6
13:56 Gerardo done
14:15 Daniel, Nutsinee to EX
- turned on green laser, adjusted Crystal Frequency to get the beat note in range, PLL locked.
- EX Lazer Hazard
15:30 Daniel, Nutsinee back
15:40 Kyle, Gerardo back from EY
15:45 Nutsinee to EY turned on Green laser. EY now Laser Hazard.
16:13 Leo finished with ESD measurement
More charge measurements. Two plots in usual style, and other couple of plots show the same measurements separately for each QUAD.
(Kyle, Gerardo)
Y-End station:
Connected and ran leak detector at turbo's exhaust in place of scroll pump, sprayed new, untested, conflats with 20 seconds of audible helium flow.
No leaks detected.
Turbo pump restored to original configuration.
Pump down continues.
Conflats tested: new Inficon gauge for ESD interlock, NEG pump 10" gate valve conflat only, Old TMDS valve + blank on middle port north door, New TMDS valve + elbow + blank on south door, and new blank for the removal of the old type gauge for ESD interlock.
Local controller shows correct voltage and current -> The signal wiring for this unit has never been correct since an additional terminal strip box was added to facilitate moving the original ion pump controller rack as required by the placement of the HEPI pump stations -> I'll consult with the EE folks
I've seen and noted this before. It has been present since early Feb when the sensors were quieted and the noise dropped enough.
If you look at trends, there is a brief upward spike on all the pressure sensor channels at the EndY HEPI Pump System that occurs everyday at 0329utc +- seconds!. Additionally, there is a weekly (Sunday) double glitch. The first glitch of the Sunday double occurs at the same time as the daily and looks similar and a second (slightly different) hits 20minutes later followed by a downward glitch 10 minutes later. Yes, every day and every Sunday.
The pressure does cause the pressure servo to react--see the CONTROL_VOUT. The glitch is actually a 40 second climb of the pressure which the servo attempts to counter with a reduction of the drive output. If the servo was driving the pressure, the sign would be reversed.
The glitches don't show in the position controllers or the inertial out of loop hepi sensors. The Actuator performance must not be that sensitive to the absolute or differential pressure. So, this really is not an IFO issue but we should figure out what is causing this. This is not seen in the other Pump Station's pressures but they may be currently too noisy.
Attached are 2 hour second trends of the daily and weekly glitches. Posting this here for the record and will open an integration issue.
Anyone else see anything at this time?
Danny Sellers, LLO Laser Safety Officer, unplugged and locked out the PSL HPO diode box power supplies to prevent the accidental activation of the High Power Oscillator.
See photo. The appropriate laser safety documentation concerning the operation of the PSL is being reviewed and updated to reflect the implementation of this new administrative/ engineering control
Note: Having the HPO diode box power supplies off does not interfere in the operation of the 35W Front End laser.
Also note that LHO made the same change today.
The adding the capability to lock out the pump diodes for the HPO is an important change in operational configuration and how we operate the sites' PSLs. For the record, this is the path followed at LHO to investigate the possibility of an engineering control (the physical locking out of power to the pump diodes), the installation of the control , and the communication with our sister site.
Date: Wed Jul 1 11:19:11 PDT 2015
Serial number: 5320
Task leader: Jason Oberling
People performing work: Jason, Rick
Facility: LHO
A lock and tag will not be used.
Period of Activity: 7/1/2015 - 7/1/2015
Area of Activity: H1 PSL, Laser Diode Room
Hazards:
Activity: In light of the event last week at LLO, to avoid accidental turning on of the PSL High Power Oscillator (HPO) we are going to test turning off the HPO diode box power supplies to see if the Front End (FE) still runs. The laser may trip during this test. In discussion with AEI Hanover, who has been talking with NeoLase, we have been told that this should be possible.
| Subject: | PSL HPO Diode Box Power Supplies Locked Out |
|---|---|
| Date: | Wed, 01 Jul 2015 12:58:38 -0700 |
| From: | Jason Oberling <oberling_j@ligo-wa.caltech.edu> |
| To: | lho all <lho-all@ligo-wa.caltech.edu> |
FYI for all:
I have turned off, unplugged, and locked out the H1 PSL HPO diode box power supplies. This is to prevent the accidental turning on of the HPO, and does not interfere with the operation of the 35W Front End laser. Lockout IDs are 3986 and 3770. If for some reason access to these power supplies is needed/desired, come see me.
Jason
| Subject: | H1 PSL HPO diode power supplies turned off and locked out |
|---|---|
| Date: | Wed, 01 Jul 2015 13:04:59 -0700 |
| From: | Jason Oberling <oberling_j@ligo-wa.caltech.edu> |
| To: | lsc-psl@ligo.org, Janeen Romie <janeen@ligo-la.caltech.edu>, Richard Oram <roram@ligo-la.caltech.edu> |
| CC: | fred.raab@ligo.org |
As the subject says, I have turned off, unplugged and locked out the PSL HPO diode box power supplies to prevent the accidental turning on of the HPO. Benno reported in this morning's PSL meeting that this should be possible and I have confirmed: having the HPO diode box power supplies off does not interfere in the operation of the 35W Front End laser. I recommend LLO implement this as soon as they are able.
Jason
Don't forget laser goggles!
ALS-X PLL is locked but not ALS-Y. I tried to change the Crystal Frequency just in case I could fix it quickly but after a few try I didn't have any luck. So, I returned the value back to where it was when I found it (-50.3570649 MHz).
I reported suspisions about the ETF (Stanford) Seismometer that is now wired up as the STS2-A or HAM2 ground sensor. That was ten days ago and here is another look from earlier this morning. Pretty much same conclusion: The ITMY and HAM5 units show very good coherence even though they are separated by 30meters. The HAM2 & ITMY sensors are just a couple meters apart and they are no showing the coherence they should: and the HAM2 & HAM5 sensors coherence is similarly poor..
While the problem may be cable or setup (level or igloo rubbing) I suspect the unit itself.
BTL: Any word on these instruments from your experiences?
If you have it insulated and it isn't rubbing, then it is probably the standard STS needs to get fixed problem, and checked that the feet are locked