Good news is that T-SAMS seems to be doing something (look at the last column of the table), so that part of the test is OK.
Single bounce (X) OMC scan shows that more than 10% is lost to 02 mode carrier at the moment. The higher the T-SAMS heating, the worse, but the heating effect is not that large (as expected).
The alignment of the beam into the IFO is questionable (I didn't do any meaningful initial alignment for corner IFO itself) and it's not impossible that the beam is clipped somewhere between IMC and HAM6. Also, is ITMX TCS good?
Slope start [UTC] | Slope end [UTC] | Heater request [W] | Thermistor2 temp [C] | C20 mean [mA] | C00 mean [mA] | 20/(00+20) |
2022/10/21 01:13:35 | 01:14:58 | 0 (still cooling) | 29.3 | 0.208 | 1.708 | 0.109 |
02:17:28 | 02:18:50 | 4.4 (still heating) | 54.8 | 0.233 | 1.670 |
0.124 |
16:41:23 | 16:42:44 | 4.4 (still heating) | 56.0 | 0.235 | 1.696 | 0.121 |
18:21:23 | 18:22:43 | 7.3 (still heating) | 72.8 | 0.250 | 1.641 | 0.132 |
20:04:09 | 20:05:30 | 0 (still cooling) | 26.0 | 0.208 | 1.698 | 0.109 |
22:14:42 | 22:16:04 | 0 | 24.7 | 0.202 | 1.691 | 0.107 |
22:20:16 | 22:21:37 | 0 | 24.66 | 0.2064 | 1.698 | 0.108 |
23:07:29 | 23:08:51 | 0 | 24.54 | 0.2025 | 1.685 | 0.107 |
What was done:
Note:
In the past, Elena's 50W and 60W single bounce scan looked more than 2 times better (alog 62883). For example, C00~67mA and C20~3.2mA for 50W X, C20/(C20+C00)~0.046.
I processed Keita's OMC scans using/ligo/gitcommon/labutils/omc_scan
, e.g. for the last scan abovepython OMCscan.py 1350428867 83 "2W input, Single bounce ITMX, OM2 heater request 0W, fifth scan" "single bounce" --verbose --make_plots -p 0.01
The results are shown in the same order as the table in Keita's alog: 1) OM2 heater 0W, first scan 2) OM2 heater 4.4W, first scan 3) OM2 heater 4.4W, second scan 4) OM2 heater 7.3W 5) OM2 heater 0W, second scan 6) OM2 heater 0W, third scan 7) OM2 heater 0W, fourth scan 8) OM2 heater 0W, fifth scan
With those processed OMC scans, I doubled checked the finesse of the OMC like we did for the scans back in April in alog 64582.
The HWHM is 0.338 MHz in Keita's measurements, and the FSR is 265 MHz, meaning the finesse is still 392, same as in April 2022.
This was done using /ligo/gitcommon/labutils/omc_scan/fit_peak.py
Keita and I looked at the 20 and 02 mode spacing for the carrier both now and in April 2022. We expected to find 0.3 MHz mode spacing between 02 and 20 modes, according to Koji's Final Design: T1000276 Table 1. We checked the numbers for our installed OMC as well, as posted in DCC T1500060 Table 25. This reports a larger mode spacing than the final design, with horizontal spacing = 58.138 MHz and vertical spacing = 57.844 MHz. This is a difference of 0.294 MHz. For 02 and 20 modes, we expect a separation of 2 * diff = 0.588 MHz. We found around 0.55 to 0.6 MHz separation between 02 and 20 for our mode scans, see the attached plots. This is in good agreement with expectation from Koji's lab measurements for our OMC. The power loss to HOMs cannot be easily read from OMC scans because of the overlapping modes. Here, we see the power in the 00 mode is 1.687 mA from the 2W omc scan fit above. The power in the 02 and 20 modes are 0.105 mA and 0.188 mA, respectively (we think).Analysis code
Code is in/ligo/gitcommon/labutils/omc_scan/fit_two_peaks.py
, should work inlabutils
conda env. We note that we forced the HWHM to be 0.335 MHz in our two-Lorentzian peak fitting routine due to some weirdness with preferring a too-high HWHM.