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Fri Oct 29 15:34:36 2010, Zach & Koji, Laser, GYRO, CCW loop characterization
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Sat Oct 30 20:02:01 2010, Koji, Laser, GYRO, gyro characterization Oct 27, 2010 (1)
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Sat Oct 30 20:18:06 2010, Koji, Laser, GYRO, gyro characterization Oct 27, 2010 (2) 
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Sat Oct 30 20:57:19 2010, Koji, Laser, GYRO, gyro characterization Oct 27, 2010 (3)
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Sat Oct 30 22:49:04 2010, Koji, Laser, GYRO, gyro characterization Oct 27, 2010 (4)
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Sat Oct 30 23:41:31 2010, Koji, Laser, GYRO, gyro characterization Oct 27, 2010 (5)
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Message ID: 1118
Entry time: Sat Oct 30 20:18:06 2010
In reply to: 1117
Reply to this: 1119
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Author: |
Koji |
Type: |
Laser |
Category: |
GYRO |
Subject: |
gyro characterization Oct 27, 2010 (2) |
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[Zach / Koji]
Measurement of the primary (CCW) cavity error / feedback signal.
Method:
- Lock the cavity. Measure the spectrum of the input monitor output.
- Close the laser shutter. Measure the same spectrum.
- Measure the feedback signal after the notch filter.
Result:
- The global shape of the error signal is a kind of flat. Though it's spiky due to mechanical resonances.
Below 10Hz it got smoother but the actual shape is not obvious because of the rough resolution.
- At around 100Hz, the error is below the dark noise. This means the out-of-loop stability does not go below the dark noise level.
Thought:
- The broad peak at around 10Hz is the servo bump.
- Note that the signal is supposed to be amplified by a factor of +41. This means the dark noise floor level is ~25nV/rtHz.
To Do:
- Calibrate these spectra in Hz/rtHz.
- How much is the optical gain in V/Hz or V/m.
- Convert this measurement into the noise budget of the Gyro signal.
- Make the unsuppressed spectrum
- => How much cavity length fluctuation does the error signal feel if there is no feedback and the sensor is infinitely linear?
- This requires the model of the open loop TF
- Compare the consistency with the same quantity derived from the feedback signal
- Compare the unsuppressed frequency noise spectra with the free running laser freq noise (see rana's phd thesis P.80).
- Convert the spectrum into the displacement noise (m/rtHz) and compare with the displacement on the table.
- Measure the shot noise level
- How much DC power do we typically have? (Actually we don't have the record during this measurement, but we can measure it again)
- Measure low frequency spectra with CDS
- How to improve the noise floor
- Is this noise level disturbing in terms of the gyro requirement? How about in the low frequency?
- How much is the demodulator noise? Put a 50-ohm terminator on the cable instead of the PD. Then measure the same signal.
- How much is the gain of the input stage. It is supposed to be +41, but we are not sure.
=> Think about the noise level at the demodulator output.
- How much is the noise level of the PD measured by an RF analyzer? Is it consistent with the above analysis?
- Do we need a new resonant RF PD? How much should we improve the noise level with the new PD? And how much noise does the new one actually have?
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