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Optical characterization (Optical characterization)
guo, gherardini, degallaix - 14:47 Monday 30 August 2021 (53000) Print this report
Repeat RTL measurement and FSR scan

The RTL measurement and the FSR of last Monday (#52945) shows some unexpected results. 

1. The lock-unlock of the north arm had the maximum reflection when cavity was locked on most of the PDs. (pic 1)

2. The lock-unlock of the west arm was too noisy, which lead to a round trip losses much lower than expected. (pic 2)

3. In the FSR scan, the 56MHz sidebands of two arms were shifted with respected to each other. (pic 3)

And the B1p PD1's shutter seemed closed during the measurement.

So in order to check if the problem is the measurement or not, we repeated most of the measurements on Friday. 

First we did lock-unlock-misalign-unlock-lock two times per arm, and checked the data, the west arm seems less noisy. But the north arm showed exactly the same pattern as Monday, so we have to understand the reason of this behaviour. 

Then we did again the FSR scan for two times, the 56MHz SB was still shifted, but since between Monday and Friday the matching of the cavities changed, so we did another 8 scans for the 'new' configuration.

In order to understand the speed limit of the scan not to cause peak distortion, we scaned the cavity with different speeds. 

All the gps of the measurements can be found in the attached file. 

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mwas - 16:10 Monday 30 August 2021 (53005) Print this report

Figure 1. I have checked that the behavior for the north arm lock/unlocks is not due to SDB1 moving. It was not the case, SDB1 was not moving following the beam as correctly NE was misaligned.

Figure 2 shows the B1p and B4 camera with the north arm locked, and Figure 3 with the north arm unlocked. The beam is indeed more powerful when the arm is locked on B1p. On B4 it is impossible to say as the integration time setting is to low to see the beam in this configuration. There is also a ghost beam ~2mm above and to the left of the main B1p when the arm is locked, which disappears when the arm is unlocked.

Figure 4 shows the B1p and camera with the west arm locked and figure 5 with the west arm unlocked. The power on the B1p camera seems also slightly higher when the arm is locked. There is no clear ghost beam in this case.

Figure 6 and 7 show the B1p camera trend when the north or west arm is locked/unlocked. There is nothing clear visible on the power channel, but the amplitude fit is clearly going up on B1p when the arm is locked for both the west and the north arm, and for the north arm the average beam position is changing (probably due to the ghost beam).

There is probably more to learn by looking at the B1p camera images in more detail.

For future attempts increasing the integration time of the B4 and B5 camera using the GxClient may show something interesting happening to the shape of the beam (or additional spots) that could explain what is happening.

 

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degallaix, guo - 11:45 Tuesday 12 October 2021 (53455) Print this report

According to the simulation shown in the attched picture, the 56MHz sideband could shift because the cavity length change. 

We checked the distance between the 56MHz sideband and the TEM00 mode normalized by the FSR, for the north arm the number is 0.4528, for the west arm is 0.4416. According to this number, the simulation gives us a 3cm shorter in the west arm cavity length.

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adf - 20:16 Saturday 16 October 2021 (53522) Print this report
From the FSR scan with the position of the sideband peaks we can also get the absolute arm length values. For example, using f2​=56MHz, and FSR=c/2L, we get: N * FSR + Delta f = f2 with N an integer. I.e. for the North arm: FSR (N + 0.4528) = f2.

With the measured offsets I get:
LN: 2999.818 m
LW: 2999.788 m

I have also done a quick Finesse 3 simulation to confirm this, see attached plot for the north arm scan. The full code is at:
https://git.ligo.org/virgo/isc/finesse/andreas_freise/-/blob/master/2021/arm_length/arm_length.ipynb
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