Elenna, Sheila
We got data today to rerun our noise budget with the current noise (150Mpc). We got quiet time with no squeezing for 10 minutes starting at 1375723813, with no large glitches. We ran excitations for LSC, laser noise, and ASC. We had quiet time with squeezing injected from the previous night of observing, I choose 1375695779 as a time with high range and no large glitches. This is commit 50358cda
Elenna, Sheila
We ran the noise budget code for this no squeezing time.
This is all commited as 0f9ffe0e
Sheila, Vicky - we have re-run the noise budget for following times:
Noise budget with squeezing. Changes here: using GDS instead of CAL-DELTAL, closer thermalized FDS time to no-sqz, using updated IFO gwinc parameters related to quantum noise calculation.
(Edit: was a glitch in the old time; updated to an FDS time without glitches. All plots updated.)
PDT: 2023-08-10 08:45:00.000000 PDTUTC: 2023-08-10 15:45:00.000000 UTC
GPS: 1375717518.000000
PDT: 2023-08-10 09:35:52.000000 PDT
UTC: 2023-08-10 16:35:52.000000 UTC
GPS: 1375720570.000000
Noise budget with no squeezing. Same time as above, now calculates using gwinc quantum noise calculation instead of semiclassical calculation used previously.
PDT: 2023-08-10 10:18:11.000000 PDT
UTC: 2023-08-10 17:18:11.000000 UTC
GPS: 1375723109.000000
Both sqz & no-sqz noise budgets now use the correlated quantum noise calculation from gwinc, instead of semiclassical calculations for SN & QRPN. The gwinc budget parameters related to quantum noise calculation are consistent with the recent sqz data set (8/2, alog 72565), with readout losses evenly split between IFO output losses that influence optical gain (20%) and SQZ injection losses (20%), parameters in plot title here. This is high on SQZ injection losses, and slightly conservative on IFO output losses. This updated FDS time is thermalized and closer to the No-SQZ time; the time used previously was several hours earlier near the start of lock, w/ ifo not yet thermalized.
Unlike before, both budgets now show GDS-CALIB STRAIN, which on 8/10 was more accurately calibrated (see Louis's alog on Aug 8, LHO:72075, comparing CAL-DELTAL and GDS vs. PCAL sweep, and his record from 72531). CAL-DELTAL was previously overestimating range due to calibration inaccuracies. We got GDS-CALIB_STRAIN data from nds servers, and at first weren't able to get input jitter data from nds, due to the sampling rate change of IMC-WFS channels from 2k to 16k, 71242. Jonathan H. helped us fix this issue, so we can now pull GDS data and input jitter data from nds.ligo-wa.caltech.edu:31200 -- thank you Jonathan!! With this, the input jitter sub-budget is kind of interesting, looks to be mostly IMC-WFS in YAW.
A quick thought on discrepancy between expected and measured DARM between below several hundred Hz-- I don't know if this could be related to the recent update to gwinc CTN parameters (high/low index loss angles), related to quantum noise, or mystery noise. The recent gwinc CTN update seemed to have dropped the calculated CTN level slightly (maybe 10-15% or so). In April 2023, Kevin helped update CTN parameters LHO:68499 to reconcile H1 budget with the official gwinc parameters, while Evan made a correlated noise measurement 68482 where noise in the bucket seems more consistent with the older CTN estimate from gwinc (or very slightly higher). Another idea is that it could be related to quantum noise, such as SRCL detuning or sqz angle which could've changed since the sqz dataset, as quantum noise can also affect the noise in this region.
All pushed as git commit 28cf2664.Edit: All pushed again as git commit 33ffd60b.
Added noise budgets with squeezing for HVAC off time on August 17 from alogs 72308, 72297.
When comparing this HVAC off time on Aug 17 with the noise budget from above on Aug 10, it's interesting to note the broadband difference in input jitter (Aug 10 vs Aug 17, HVAC off). Between these times, worth noting that I think there were several additional improvements (like LSC FF or SUS-related) as well.
Edit: updated 8/10 input jitter budget to the less glitchy noise budget time.
Much of the gap between expected DARM (black traces) and measured DARM (red traces) in the noise budget looks compatible with elevating the CTN trace. Budget plots with 100 Hz CTN @ 1.45e-20 m/rtHz are attached below for the no-HVAC times. This is almost 30% higher than the new gwinc nominal CTN at 100 Hz (i.e., 1.128e-20 m/rtHz --> 1.45e-20 m/rtHz). Compared to the old gwinc estimate of 1.3e-20, this is ~11% higher. Quantum noise calculation unchanged here.
This CTN level is similar to the 30% of excess correlated noise that Evan H. observed in April 2023, see LHO:68482. His cross-correlation measurement sees ~30% excess correlated noise around 100 Hz after subtracting input jitter noise, where that "30%" is using the newer gwinc CTN estimate of 1.128e-20 m/rtHz @ 100 Hz. This elevated correlated noise, if attributed to CTN, corresponds to CTN @ 100 Hz of about 1.3*1.128 = 1.46e-20 m/rtHz. See this git merge request for the gwinc CTN update ; this update lowered the expected CTN at 100 Hz by ~15%, from 1.3e-20 (old) to 1.1e-20 m/rtHz (new), based on updated MIT measurements.
For reference, I have plotted these various CTN levels as dotted traces in the thermal sub-budget.
To elevate CTN levels by 30% in the budget code, I scaled both high+low index loss angles by a factor of 1.8, specifically Philhighn 3.89e-4 --> 7e-4 ; Phillown 2.3e-5 --> 4.14e-5. It seems like much higher than this level ~1.45e-20 might be difficult to reconcile with the full budget.
Noteworthy w.r.t. squeezing: from the laser noise sub-budget, laser frequency noise looks within 33% of squeezed shot noise with ~3.7dB of squeezing. By contrast, the L1 noise budget from Aug 2023 (LLO:66532) shows laser noise at the ~20% level of squeezed shot noise with 5.3 dB of squeezing -- i.e. a lower laser noise floor past shot noise.
The following plots can be found in /ligo/gitcommon/NoiseBudget/aligoNB/out/H1/lho_all_noisebudgets_081723_noHVAC_elevatedCTN, and not yet commited to the git repo.
Plots with higher CTN are attached here for the SQZ / no-SQZ proper noise budget times from 8/10, when injections were run.
Comparing the sqz vs. no-sqz budgets suggests there might be more to understand here, to tease apart the contributions from coating thermal noise (CTN) vs. quantum noise in the bucket. In particular, something disturbing that stands out, is that I imagined that if elevated CTN is the physical effect we're missing, it would reconcile both NBs with and without squeezing. However, there is still some discrepancy in the un-squeezed budget, which was not resolved by CTN, and seems to have a consistent shape. I'm wondering if this is related to the IFO configuration as it affects the quantum noise without squeezing. I think this could result from a non-zero but small SRCL detuning since it looks like elevated noise, with a clear shape, that increases below the DARM pole. Simply elevating CTN to match the no-sqz budget would put us in conflict with squeezed darm, so I don't think it makes sense to elevate CTN further. The budget currently has 0 SRCL detuning as it "seems small-ish", but this parameter is somewhat unconstrained in the quantum noise models.
In models, the readout angle is upper-bounded by Sheila's contrast defect measurement, though in principle it could probably be anything lower than that too, which could be worth exploring. It might be helpful to have an external measurement of the thermalized physical SRCL detuning, or in the models allowing the SRCL detunings to vary, to explore how it fits or is constrained by the fuller noise budget picture.
Plots with squeezing can be found in /ligo/gitcommon/NoiseBudget/aligoNB/out/H1/lho_all_noisebudgets. No squeezing plots are in /ligo/gitcommon/NoiseBudget/aligoNB/out/H1/lho_darm_nosqz_noisebudget.
I pushed to git commit 70ca191c without elevated CTN and the associated extra traces. The relevant parameters are left commented out at the bottom of the QuantumParams file, and relevant code to plot the extra traces is commented out in the lho_all_noisebudgets script.