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AdV-ISC (Commissioning up to first full interferometer lock)
mantovani, pinto - 14:56 Thursday 28 April 2022 (55643) Print this report
Double cavity pole measurement with 1 excitation line on DARM @ 314.3

The double cavity pole monitor is fundamental for the ITF characterization. It can be measured by monitoring the high frequency region of the DARM OLTF.

As it is visible the OLTF of darm changes with different double cavity pole frequencies, see Figure 1 from 200Hz to 450Hz.

The phase value can be used to extract the cavity pole frequency, see Figure 2. From this behavior the calibration can be found and the signal can be extracted as it is visible in Figure 3.

 

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mwas - 20:05 Friday 10 June 2022 (56115) Print this report

A simple response has a shape of

\frac{1}{1 + i \frac{f_L}{f_p}}

where f_L is the frequency of the line used for the measurement and f_p is the frequency of the pole.

This means that a priori the transformation of phase to pole frequency should be

f_p = -\frac{f_L}{\tan(\phi - \phi_0)}

with \phi_0 some phase offset at the line frequency due to other reasons.

Figure 1 shows that the fitted exponential overlaps very well with the formula above when using the injected line frequency of 314Hz and a phase offset of 2.415 radian.

Figure 2, if ones start to expand the range considered the two curves stop overlapping, for pole frequencies below 200Hz.

At the end, it should not matter much which function is used for the conversion in this application. Using the inverse of the tangent is more satisfactory intelectually, and it may lead to less issues computationally. Because the exponential function can be slow in some cases, and lead to a less stable time for finishing each real time computation cycle.

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