Here are the X1 and X2 module pressures while the tube washing has been progressing. The features present are those resulting from ION pump voltage changes, gate valve cycles, and a repair of a leaky metal valve at XEND.
Rick Savage and the Pcal Team request NO IFO LIGHT IN THE ARMS while they are at the end stations doing calibration work. This activity will take approx 2 hrs or until they report to the operator. (whichever comes first). That is all.
Calibration run ends today at 12:01PM
Annealing begins today at 12:01PM
SUS - no report
SEI - no report
Pcal - Rick and co. finishing calibration efforets at both end stations. Mirrors will remain in nominal states w/ no shaking. Only alognment of pcal will take place.
FAC - Issues with RO water ongoing. Installation of aluminum strips wil begin today
Jim batch announced an upcomin computer upgrade for FOM monitors. MAC mini will be replaced with Intel nook. (possibly video4)
Vern mentioned re-implementation of Betsy's LockLoss Pie chart to track destructive ground motion around the site.
CDS model and DAQ restarts during the first three days of the ER7 period.
* = unexpected restart
model restarts logged for Tue 26/May/2015
2015_05_26 11:22 h1susetmy
2015_05_26 11:27 h1hpiham4
2015_05_26 11:27 h1hpiham5
2015_05_26 11:27 h1iopseih45
2015_05_26 11:27 h1isiham4
2015_05_26 11:27 h1isiham5
2015_05_26 11:45 h1broadcast0
2015_05_26 11:45 h1dc0
2015_05_26 11:45 h1fw0
2015_05_26 11:45 h1fw1
2015_05_26 11:45 h1nds0
2015_05_26 11:45 h1nds1
2015_05_26 17:02 h1fw1*
2015_05_26 20:06 h1fw1*
model restarts logged for Wed 27/May/2015
2015_05_27 08:27 h1iopsusb123
2015_05_27 08:27 h1susbs
2015_05_27 08:27 h1susitmx
2015_05_27 08:27 h1susitmy
model restarts logged for Thu 28/May/2015
2015_05_28 01:56 h1fw0*
2015_05_28 06:17 h1fw1*
2015_05_28 12:44 h1calcs
2015_05_28 12:44 h1calex
2015_05_28 12:44 h1caley
2015_05_28 12:46 h1broadcast0
2015_05_28 12:46 h1dc0
2015_05_28 12:46 h1fw0
2015_05_28 12:46 h1fw1
2015_05_28 12:46 h1nds0
2015_05_28 12:46 h1nds1
2015_05_28 13:04 h1iscex
2015_05_28 13:08 h1calex
2015_05_28 14:45 h1calex
2015_05_28 14:57 h1calex
2015_05_28 15:22 h1calex
2015_05_28 15:22 h1caley
2015_05_28 15:24 h1calcs
2015_05_28 15:34 h1broadcast0
2015_05_28 15:34 h1dc0
2015_05_28 15:34 h1fw0
2015_05_28 15:34 h1fw1
2015_05_28 15:34 h1nds0
2015_05_28 15:34 h1nds1
- 4 locks that made it far enough to produce a range, though the calibration is currently inacurate, and so is range
- first CW injection of aLigo, see Eric Thrane's alog #18681
- bounce mode on ETMX and sometimes ITMX a problem, and Jeff and I reduced the gain on ETMX manually several times, so Evan has reduced the gain that Guardian sets
- tidal on ETMX was off, and is now on
- collecting templates - Sheila gave ops a few new ones which are in the ops/Templates directory
- IFO is unlocked and leaving it with Evan and Jeff
E. Hall, J. Kissel, C. Vorvick The 7.0 Mag EQ in Chirikof Island, AK hit the IFO hard, and has ended activity for the night. Almost all SEI and SUS have tripped, and we've left before the ground was settled enough to untrip them. We'll leave it up to morning crew to recover.
D. Barker, J. Batch, K. Izumi, S. Karki, J. Kissel, R. Savage, D. Tuyenbayev, C. Vorvick
We've finished the bulk of the invasive calibration work today. The PCAL team needs a little bit more time tomorrow, but they'll come in early such that they're finished before 12p PT. Here's a recap of this past day's activity:
J. Kissel, K. Izumi
Retook free swinging Michelson measurements, this time using ETMX ESD and the Full DC Readout DARM sensor as another middle man to propagate the ITM drive to MICH [m] through to all three stages of ETMY. Preliminary results from yesterday indicate good agreement between model and measurement for at least ETMY L2 between 4-7 [Hz], with the statistical uncertainty and measurement scatter blowing up below 4 [Hz]. (Detailed analysis and aLOG to come)
K. Izumi
Adding ETMX L3 drive to ALS DIFF to the collection of transfer functions so we can propagate the ALS DIFF VCO calibration to ETMY using the same ETMX to DARM and ETMY to DARM TFs taken for the above free-swinging MICH. (Detailed analysis and aLOG to come)
J. Kissel, D. Barker, J. Batch
Updated the CAL_INJ_MASTER, PCAL_MASTER, and CAL_CS_MASTER library parts to
- obtain some updates to the hardware injection infrastructure for GRB alerts and well-commissioned ODC vector,
- add a monitor channel after the ring buffer of the CAL-CS actuation chain
- add infrastructure to use ITMs as DARM actuators into the DARM actuation calibration path
- change the blind injection filter bank to be named "BLIND" instead of "BLND",
- add infrastructure for eventually computing a optical gain correction coefficient in the corner station using PCAL lines*
*see details in LHO aLOG 18671
E. Thrane, J. Kissel, C. Vorvick
Tested CW Hardware Injections; see LHO aLOGs 18681 and 18682.
Goals for tomorrow:
J. Kissel, K. Izumi
Finish processing the ALS DIFF and Free Swinging MICH assessments of the ETMY actuation strength, and update DARM model accordingly
J. Kissel
Process DARM OLG TF from LHO aLOG 18662, and compare against new DARM model
J. Kissel, K. Izumi
Update CAL-CS front end calibration to account for new Low Noise ESD driver strength and new L1, L2, L3 actuation scheme, and shift down the DARM coupled cavity pole frequency to our best measured of 355 [Hz] instead of 389 [Hz].
R. Savage, S. Karki, D. Tuyenbayev
Complete measurements of photodiode frequency response at both End Stations.
J. Kissel, R. Savage, K. Izumi, S. Karki, D. Tuyenbayev
Measure PCAL to DARM transfer functions for both end stations, begin to develop a model for the transfer function to inform sensing function scale coefficient, independent measure of cavity pole frequency, etc. etc.
Chris B, Jeff, Eric Starting at GPS = 1116915517, we turned on the HWINJ with gain=10 to run in the background indefinitely. The idea is to make the CW signal loud enough that CW can recover some of these signals with just a few days of data, but weak enough so that they don't disturb the strain spectrum significantly. If these jobs are found to cause a problem with anything, simply disable the injections with the off switch in the cal model. NOTE: the overall injection gain is now set to 10, so any tinj injections should be scaled DOWN by 10x. Here are the CW signals that are currently active (frequency and amplitude shown below not including gain=10 factor): -bash-4.1$ grep Freq *cfg Pulsar0_StrainAmp.cfg:Freq = 265.5771052 ## GW frequency at tRef Pulsar1_StrainAmp.cfg:Freq = 849.0832962 ## GW frequency at tRef Pulsar2_StrainAmp.cfg:Freq = 575.163573 ## GW frequency at tRef Pulsar3_StrainAmp.cfg:Freq = 108.8571594 ## GW frequency at tRef Pulsar4_StrainAmp.cfg:Freq = 1403.163331 ## GW frequency at tRef Pulsar5_StrainAmp.cfg:Freq = 52.80832436 ## GW frequency at tRef Pulsar6_StrainAmp.cfg:Freq = 148.7190257 ## GW frequency at tRef Pulsar7_StrainAmp.cfg:Freq = 1220.979581 ## GW frequency at tRef Pulsar8_StrainAmp.cfg:Freq = 194.3083185 ## GW frequency at tRef Pulsar9_StrainAmp.cfg:Freq = 763.8473165 ## GW frequency at tRef Pulsar10_StrainAmp.cfg:Freq = 26.3589129 ## GW frequency at tRef Pulsar11_StrainAmp.cfg:Freq = 31.4248598 ## GW frequency at tRef Pulsar12_StrainAmp.cfg:Freq = 39.7276097 ## GW frequency at tRef -bash-4.1$ grep aPlus *cfg Pulsar0_StrainAmp.cfg:aPlus = 2.0125e-25 ## plus-polarization signal amplitude Pulsar1_StrainAmp.cfg:aPlus = 6.4405e-25 ## plus-polarization signal amplitude Pulsar2_StrainAmp.cfg:aPlus = 3.74175e-24 ## plus-polarization signal amplitude Pulsar3_StrainAmp.cfg:aPlus = 8.1915e-24 ## plus-polarization signal amplitude Pulsar4_StrainAmp.cfg:aPlus = 2.45645e-23 ## plus-polarization signal amplitude Pulsar5_StrainAmp.cfg:aPlus = 2.94475e-24 ## plus-polarization signal amplitude Pulsar6_StrainAmp.cfg:aPlus = 3.54275e-25 ## plus-polarization signal amplitude Pulsar7_StrainAmp.cfg:aPlus = 1.728625e-24 ## plus-polarization signal amplitude Pulsar8_StrainAmp.cfg:aPlus = 7.9815e-24 ## plus-polarization signal amplitude Pulsar9_StrainAmp.cfg:aPlus = 5.6235e-25 ## plus-polarization signal amplitude Pulsar10_StrainAmp.cfg:aPlus = 2.343323e-024 ## plus-polarization signal amplitude Pulsar11_StrainAmp.cfg:aPlus = 9.958896e-024 ## plus-polarization signal amplitude Pulsar12_StrainAmp.cfg:aPlus = 1.331275e-025 ## plus-polarization signal amplitude
One thing to watch out for is that for the sake of continuity with initial LIGO HW injections (cf. Emerson, consistency, hobgoblins), we use reference times going back to the start of S3, and some of the stars are spinning down pretty hard. The parameters for this set of injections, including the ER7 start and stop frequencies in the source rest frames can be found here. (Those frequencies can be further modulated by Doppler effects from the Earth's rotation and orbital motion, but for the duration of the ER7 run, those effects are no greater than 1/100,000.) In particular, the start-of-ER7 source-frame frequencies for the 13 pulsars are the following, where especially large spin-downs are noted: 0 - 265.575587774 Hz 1 - 848.973602759 Hz 2 - 575.163522907 Hz 3 - 108.857159395 Hz 4 - 1393.875953 Hz (vs 1403.163331 Hz in S3) 5 - 52.8083243585 Hz 6 - 146.258236176 Hz (vs 148.7190257 Hz in S3) 7 - 1220.57005882 Hz (vs 1220.979581 Hz in S3) 8 - 191.145490954 Hz (vs 194.3083185 Hz in S3) 9 - 763.847316495 Hz 10 - 26.3430397679 Hz 11 - 31.4247651214 Hz 12 - 38.5604676312 Hz (vs 39.7276097 in S3) I checked the 15 minutes or so of data from last night, preceding the Alaskan earthquake, where all pulsars were turned on. Not all of them were immediately visible, but attached are spectrograms for some that were obviously there (the NDS2 server is giving me trouble at the moment; I'll look for more signals later).
NDS2 is cooperating again. Here are spectrograms for additional visible CW injections in last night's pre-quake lock.
Cheryl, Jeff, Eric We carried out the first successful demonstration of CW injection with aLIGO. Previously, we have tested the injection code, but we hadn't been able to confirm that the injections were making it into the detector. Cheryl and Jeff put H1 in a low-noise DC state with ~30 Mpc inspiral range. The intent bit was turned on. We turned on the injections at 22:19:20 to confirm that the excitation showed up in the filter bank. However, the injection amplitudes are too weak to show up by eye in the spectrum (by design) and so we prepared to increase the amplitude. For the second test, which started at 22:26:44, we made one of the injections 10x louder than the others so it would show up as a sharp line. We chose to carry out the test with Pulsar #0, which has a frequency of f0 = 265.5771052 Hz and a strain amplitudes of aPlus=2.0125e-25, aCross=1.960625e-25. We increased these values of aCross and aPlus by a factor of ten and restarted the injections. Jeff could not see them by eye in the control room spectrum. We increased the gain on the injection channel until we Jeff could be absolutely sure he saw a CW line. (For CW/detchar people looking at this data, you will see the signal get louder according to step function factors of ten.) Jeff could clearly see the line when we set the gain to 200, corresponding to strain of ~2e-25 x 10 x 200 = 4e-22 or displacement of 1.6e-18m. We confirmed that the measured displacement approximately matched the value predicted by the pulsar injection configuration file. We turned off the injections in order to restart them with a lower amplitude. However we lost lock before we restart. The injections ended sometime not long after GPS = 1116912836. In the course of this test, we found a good preliminary value to use for the HWINJ LIMIT. In order to avoid clipping, we set LIMIT=200. This allowed us to create a strong line. The output of the control loop during this time was O(10,000). I suggest that we use LIMIT=200 as a new default and see if that gives us enough range for our transient injections.
At 2:18:50 UTC the IFO reached LSC_FF and I engaged the Intent Bit as a test, since Jaime had just had me load new code into the ISC_LOCK guardian, that will unset the Intent Bit at lock loss.
NOTE: This lock stretch IS NOT at about 60Mpc - the calibration is KNOWN TO BE INACCURATE, and is being worked on.
ETMY ESD is saturating constantly, so while I set the Intent Bit as a test, this lock stretch is of QUESTIONABLE USE for data analysis.
2:32 UTC, lock loss and Intent Bit is still green, calling Jaime.
Hopefully addressed. See comment to previous post.
It has been decided that for ER7 the OBSERVATION INTENT bit shall be UNSET after every lockloss, thereby forcing the operator to manually re-enable to the bit each time full lock has been achieved and the operator has deemed the detector "observation ready".
I have modified the LOCKLOSS state in the ISC_LOCK guardian to set H1:ODC-OPERATOR_OBSERVATION_READY to zero:
class LOCKLOSS(GuardState):
index = 2
request = False
def main(self):
ezca['ODC-OPERATOR_OBSERVATION_READY'] = 0
return True
This change has been committed to the USERAPPS svn, but the ISC_LOCK node has not been reloaded. Someone (e.g. operator) should hit LOAD on the ISC_LOCK guardian to make this change take affect.
This is meant to be an ER7 hack only. The handling of the OBSERVATION INTENT bit will be reviewed after ER7, and a better, more structured handling of this bit (and of other modal bits) will be implemented ahead of O1.
I just spoke to Cheryl, the on duty operator, about reloading the ISC_LOCK code. While I was on the phone, she hit LOAD on the ISC_LOCK guardian control screen, and the code was reloaded without issue. We should watch to make sure that ISC_LOCK does the correct thing to unset the bit on the next lockloss.
The last change didn't take because of a little guardian subtlty. The ISC_LOCK:DOWN state is a "goto" state, which means the LOCKLOSS state experiences a "redirect" before it even executes any code. I added the "redirect = False" flag to the LOCKLOSS state which ensures that it is executed in full before the redirect.
The code was reloaded, so we're again waiting for a lock->intent->lockloss cycle to confirm that things are working.
Pcal Team,
The displacement calibration factor that converts the TxPD (photodiode that measures a small amount of sampled light going to the ETM) and RxPD (photodiode that measures all of the reflected light from the ETM) readings into metres are now reported in DCC document # T1500252.
We have calibrated photon calibrator at each end-stations (both LHO and LLO) multiple times after installation. This document contains all the calibration factors obtained on different dates. However, the numbers obtained at different dates for each endstation are within a percent of each other when they were measured under "identical conditions". There has been some optical layout changes in the Transmitter module (described in LHO alog #17145 ) which has resulted in different displacement calibration factor for TxPD over time as you will notice in the table in DCC document linked above. But these numbers are consistent with the changes that were made.
For RxPD, the calibration factor at LHO has been measured consistently within 1% percent. However, we noticed recently that LLO had their calibration factor differ from LHO by about 20%, although the calibration numbers from different dates for same end-station agreed within a percent. We were not sure about why the sensitivity of these detector were different despite the components being same. This should not effect the calibration but we nonetheless replaced those two RxPD at LLO with two spare RxPD and now the calibration numbers at LLO are comparable with LHO. So the latest calibration number for RxPD from LLO is about 20% more than what it usually has been.
Recently, we noticed some power variation in the RxPD signal (while TxPD stays flat) and also variation in optical efficiency. We are actively looking into this issue and have some leads. We will put an alog about it soon. However, this should not alter the calibration factor by more than a few percent at its max.
Added 747 channels. Removed 36 channels. All were calibration channels.
Jeff, Jim, Dave
The h1calex, h1caley models were changed to add RFM sender IPC parts. The h1calcs model was changed to add two receivers for these channels. When the new code was ran, random single and sometimes double errors were seen at the receiver for these channels at a rate of about one per minute from both end stations.
Working on the X-Arm, our first test was to turn off the h1iscex model, which has 8 RFM senders, to check if the addition of one channel has exceeded a limit. The CAL error rate was unaffected.
We noted that both h1iscex and h1calex are processing for about the same length of time (6uS and 5uS respectively). We thought that therefore the models are writing to the RFM card in h1iscex at roughly the same time. The h1lasex model, on the other hand, is writing to the RFM card at the 33uS mark.
We delayed the execution of h1calex by modifying the PCAL_MASTER.mdl model and adding a bunch of filter modules. Jim created filters to run on these FMs to slow down the model. Our first try did not delay by much (cpu about 10uS) and the error rate was about the same. Our second try delayed too much, to about 33uS and the error rate shot up to hundreds per second. Our third try put the cpu time to 25uS which is what we wanted. Unfortunately the receive error rate was unaffected.
At this point we were considering sending the channel over the the ISC model via shared memory and letting that model RFM the channel to the corner station (similar to what ODC is doing). Jeff decided at this point to remove the new IPCs for now.
To back the change out, we did the following:
Dan, Evan, Sheila
Tonight we started to look at the angle to length couplings of our test masses. We injected lines into pitch and yaw on the PUMs, and adjusted the A2L gains to minimize them. Using the math in the 40 meter alog and Jax's alog, we can estimate the miscentering from these measurements
| Gain P2L | vertical miscentering (mm) | Gain Y2L | horizontal miscentering (mm) | |
| ETMX | 1.6 | 21 | 1.1 | 14.4 |
| ETMY | 0.69 | 9 | -0.3 | -3.9 |
| ITMX | 2.4 | 31.5 | 1.15 | 15 |
| ITMY | 1.5 | 19.7 | N/A (-1.7 to -2) |
After we had adjusted these, we saw an improvement in the spectrum below 20 Hz. The line in the attached screen shot at 16.6 Hz with sidebands at half a hertz are the excitation. Keep in mind that this is on the new ESD driver and we haven't redone the calibration yet, but clearly this improved the noise below 20 Hz.
Earlier in the evening we were having difficuulty powering up because of a pitch instability at the main suspension resonant frequency that showed up in all the test masses. We moved the QPD offsets for pitch back to what they were may 15th, (they had been changed last tuesday). We then remeasured the miscentering for pitch only, things were a little bit better. Once we increased the power to 17 Watts, the IFO was stable and we repeated some of the measurements. We were able to power up to 23 Watts without seeing the instability twice, but lost the lock quickly for other reasons.
| Gain P2L | vertical miscentering (mm) | 17 Watts P2L | ||
| ETMX | 0.7 | 9.18 | 0.8 | |
| ETMY | -0.57 | -7.5 | -0.49 | |
| ITMX | 2.1 | 27.6 | 2.4 | |
| ITMY | 1.2 | 15.7 | NA |
DARM OLTF file attached. This template has reduced drive strength so that the ESD does not saturate in the LVLN state.
At last I was able to switch the DARM actuation over to ETMY at 25 W with the LPF engaged on the LVLN driver. We had discovered that the L1 LOCK filters on the ETMs were charging up because of small amounts of ringing in the lower stage filters. Therefore, the L1 filter for ETMX is zeroed after actuation is moved to ETMY, and the lock filters for ETMY are cleared after lockloss. Also, the INCREASE_POWER state now automatically increases the power to 25 W once again.
I tried the LOWNOISE_ESD_ETMY state at 25 W once, and it seemed to work. I then turned on some pieces of the LSC_FF state (namely the SRCL gain reduction, the SRCL cutoff, and the MICH FF). I am leaving the IFO locked with the intent bit undisturbed.
One last note: the power was 3 Watts in the spectrum attached, and to repeat, the calibration is not updated since the actuator change. They're working on it
The displacements in mm are wrong here, we were measureing from the PUM.
Another DARM OLTF, this time with the ETMY LPF off.
There are two DARM Open Loop Gain TFs attached as comments to this entry that represent the first two DARM OLGTFs taken with the new low noise ESD driver and the new L1L2L3 hierarchical control scheme. I've downloaded them and submitted them to the CalSVN for use later: - From LHO aLOG 18662, DcDarmLVLN.xml, measured starting 2015-05-28 13:17:00 UTC, has been copied to /ligo/svncommon/CalSVN/aligocalibration/trunk/Runs/PreER7/H1/Measurements/DARMOLGTFs/2015-05-28_H1_DARM_OLGTF_LHOaLOG18662_ETMYL3LPON.xml - From LHO aLOG 18709, DcDarmLVLN.xml, measured starting 2015-05-30 03:07:00 UTC, has been copied to /ligo/svncommon/CalSVN/aligocalibration/trunk/Runs/PreER7/H1/Measurements/DARMOLGTFs/2015-05-30_H1_DARM_OLGTF_LHOaLOG18709_ETMYL3LPOFF.xml. I attach conlogs of all relevant DARM filter banks and BIO switches, where the date in the file name corresponds to each measurement.