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PEM (Center)
takaaki.yokozawa - 9:42 Tuesday 11 February 2025 (32631) Print this report
Noise projection from IMMT1 trans QPD to DARM
I measured the transfer function from IMMT1 TRANS QPD2 PIT/YAW to DARM with the vibration of the IFI chanber floor using the large shaker (klog32613)
Fig.1. showed the results (Previous one was written in klog32007, there is not so large change)

I also performed the noise projection with same manner of the klog32588
The result can be seen in Fig.2.

I noticed the several frequency conversion during the injection as shown in Fig.3.
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takaaki.yokozawa - 10:57 Tuesday 11 February 2025 (32636) Print this report
I also measured the transfer function with the with the vibration of the IFI chanber bellowsleg using the small shaker1 (klog32613)
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tatsuki.washimi - 21:41 Thursday 13 February 2025 (32672) Print this report

[R.Sato, Washimi]

We analyzed the swept sine shaker injection test for the IFI chamber's bellows leg performed on Feb. 11 (klog32636).

Even though the excited lines in the seismometer signal were narrow, the excess in the strain signal got wider around the injected frequencies.

Moreover, the strain signals around 60 Hz were also excited when the shaker oscillated around 120 Hz.

These results mean the couplings from the ground vibration to the strain are non-linear and transfer functions are inappropriate for estimating the noise budget.

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tatsuki.washimi - 20:53 Friday 14 February 2025 (32693) Print this report

[R.Sato, Washimi]

We also analyzed the swept sine shaker injection test for the IFI floor using the large shaker performed on Feb. 11 (klog32636).
Similar to the results of the small shaker injection (klog32672), the excess in the strain signal got wider around the injected frequencies.

On the other hand, the unnatural excess around 50-60 Hz was not found. So It was due to an accidental coincidence in the measurement timing.

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tatsuki.washimi - 21:09 Friday 14 February 2025 (32694) Print this report

[R.Sato, Washimi]

We changed the target channel from the strain to the IMMT1 trans-QPD (pitch).

The excess in the trans-QPD signal was very narrow at the injected frequencies. So the noise path 
       floor -> in-vac table -> input STMs -> beam sitter
is the liner coupling and the non-linear processes happen after them.

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