Summary
As already known, the spectral bumpy structure in DARM at around 117 Hz would be due to the angular jitter of the input beam. What is strange is that the corresponding bumps at IMMT1T seems only grown during PRFPMI locked, and not found when it is down. Considering the control topology, this should not happen. This post is to show the points by creating the attached figures.
Details
Fig. 1 shows projection from IMMT1T QPDs (K1:IMC-IMMT1_TRANS_QPDA{1,2}_DC_PIT_OUT_DQ
) to DARM (K1:CAL-CS_PROC_DARM_DISPLACEMENT_DQ
) made with the same transfer function (-4*x^2; in other words, I reused this same transfer function) introduced in 24187 in the silent run on Mar. 21 00:00:00 UTC (see 24475). In fact the S/N of the QPD output is better for QPD2 than that of QPD1, but the transfer function was of QPD1, so I plot both; these QPDs show slightly different gain seemingly. Anyway, It is obvious, at least the 117 Hz bumpy structure, the 128 Hz stable peak, and the 163 Hz bump would be related to the angular jitter of the input beam that can be detected with these IMMT1 transmission QPDs. This has been already known since 24187.
The strange thnig is related with the fact already reported in 24529. To repeat the point, Fig. 2 shows that the bumpy structures around 117 Hz and 163 Hz get larger when PRFPMI locked (or, during the silent run, of Mar. 21 00:00:00 UTC), while they are less when the interferometer is down (of Mar. 21 02:00:00 UTC) but IO Gurdian is in PROVIDING_STABLE_LIGHT
. So, the question is why these bumpy structures appear in IMMT1T QPDs when the interferometer locked? Understanding the mechanism how the bumps appear in the QPDs will make DARM better, I guess.
The first scenario might be due to some coupling from MCL feedaround during PRFPMI locked. Fig. 3 shows the relevant signals, but there are no coherence with the 117 Hz bump in IMMT1T QPD and MCE input signal, while there is strong coherence around 127 Hz, which is we know a stable peak found in DARM, IMMT1T, and CARM-related signals (but may be not so related to the current issue, although we love to damp it...). Then, whar is the next candidate of the scenario...???
Anyway, the other things I noticed in Fig. 3 are
- Why the 60 Hz power line (maybe) and its hramonics are only seen when down?
- Strong coherence below 20 Hz. Do we need more diagonalization of P/L for the MCE suspension? Is there possibility that this unwanted pitch input may have upconversion to 117 Hz? Indeed there are several other bumps found in IMMT1T when PRFPMI locked. For reference Fig. 4 is wider version of Fig. 3. Do we already have a measured transfer function from MCL excitation to DARM?
By the way the other peaks in IMMT1T that are not correlated with DARM seems to be due to the fluctuation of the pylon; they have strong coherence with IMMT1T oplev signals at these peaks.