Yesterday we started to work on the IPATSIA after the installation in the CEB area, currently on the WI tower.
We switched on the CO2 laser at 9:55 UTC, waiting some time for the laser thermal stabilization at around ~50mW of injected power.
We then started shining the mirror at 11:22 UTC with the ITF in LN2 since ~10:00UTC (BS put in full BW manually each time). To be noted that during the first part of the LN2, the SR has yet to recover the aligned position because of the needed disalignment trick to reduce B1p power. Its regime state is reached several minutes later.
Fig. 1 shows the thermal image of the mirror before the PA (ITF locked) and Fig. 2 shows the image after we started shining the mirror in the first position. In Fig. 3 we have the same position, after one hour of shining, with a different palette, that we used for the rest of the images. As we can see in the two figure, a simmetric spot (wrt the mirror center) appears together with the CO2-PA. This is similar to what we found in one of the position at the WE (see fig. 4 in #67670), and not understood yet.
Right after the injection of the CO2-PA, we had a huge instability of the ITF because of a glitch on the SR_AA signals and, as a consequence, OMC alignment. The effect of the CO2-PA was anyway visible with an almost ~9% of reduction of the power circulating into the arms. The DCP moved away and came back only after ~22 minutes.
In this position, the CMRF was very high and the sidebands very low. After two hours of lock, we tried to compensate adding offset on the BS_AA. Unlike what usually happens, adding offset on the TY didn’t help at all. Changing the BS_TX_SET in the negative direction did help, but it also increased the B1p power. With the BS_TX_SET, the ITF was even more unstable (see Fig. 4).
At 14.15 UTC we stop moving the BS, the CMRF was quite ok and we wait there for some time to acquire data in this condition. The offset has been removed at 14.45 UTC.
We than moved directly the CO2-PA to another point (10k picomotor steps in the vertical lower direction, the camera being upside down, which should correspond roughly to 8mm w.r.t the previous position). At 14.52 UTC we started shining in the second position (see Fig. 5). We waited there for half an hour to acquire data.
At 15.30 UTC we moved again the CO2-PA from the same amount as before in the vertical direction, adding another ~8mm (see Fig. 6), but the ITF unlocked immediately after. We stoped shining at 15.32h and we waited the ITF to lock in LN2 again.
At 16.45 UTC we started shining again in the third position, after the ITF recovered the LN2 state but at 17.00 UTC the ITF unlocked again and we turned up the flip mirror and stop shining the CO2-PA. We tried one last time to recover the ITF to acquire some data, started shining at 17.56 UTC but at 18.06 UTC the ITF unlocked again and we stopped there.
Fig. 7 shows a summary of the main DoF of the entire shift, till the last unlock.
Few comments:
- Working on the input mirrors seems to have a stronger impact on the ITF, mainly on the CMRF and on the sidebands. Estimating the amount of 1/f^2/3 noise will be more complicated.
- At each injection of CO2-PA, whatever the position, the DCP estimation changed (both the ISC and the Hrec one). Only for the first position it happened together with a glitch on the SR AA which eventually caused an instability of the ITF. The DCP took several minutes to recover its value, and the same for the BNS range (see Fig. 8). This effect seems to correlate well with the SR_TY position. Arm power and sidebands are not affected.
- The CMRF and the othere DoF are less affected by the CO2-PA as far as we go away from the center of the mirror. However, for the last position the lock lasted barely few minutes (only 1' the first time and less than 15' in the last two attemps). The ITF was quite robust either before and after this position (it remained locked all the night long).
This may indicate that we excite some instabilities once in this position (some specific HOM?).