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Entry  Sat Mar 12 05:32:40 2011, Zach, Laser, GYRO, current gyro noise gyro_noise_with_contribs_3_11_11.pngoutput_box.pnginput_box.png
    Reply  Sat Mar 12 16:11:35 2011, Koji, Laser, GYRO, current gyro noise 
       Reply  Sat Mar 12 16:22:53 2011, Zach, Laser, GYRO, current gyro noise 
          Reply  Sat Mar 12 19:20:19 2011, Koji, Laser, GYRO, current gyro noise 
             Reply  Sat Mar 12 21:24:14 2011, Zach, Laser, GYRO, current gyro noise OLTFs_3_11_11.png
                Reply  Sun Mar 13 00:27:29 2011, Koji, Laser, GYRO, current gyro noise 
Message ID: 1348     Entry time: Sat Mar 12 16:22:53 2011     In reply to: 1347     Reply to this: 1349
Author: Zach 
Type: Laser 
Category: GYRO 
Subject: current gyro noise 

This is the answer I would give:

  • The magnitude is lower because the differential noise of the input optics is suppressed by the secondary (CW) loop gain in the PLL readout (but not in the AOM readout). This was the main advantage to this readout scheme in the first place (see this post)
  • The shape above ~100 Hz is different either because the residual primary loop noise ("spillover noise") is also suppressed in the PLL readout OR because the PLL bandwidth is lower than this. We don't have an OLTF of the PLL yet, but we can see which one it is by carefully reviewing the diagram in the above post to see if the spillover noise should indeed be suppressed (we didn't think it would).

Quote:

Why the AOM actuation (blue) and the PLL actuation (green) different so much?

Quote:

gyro_noise_with_contribs_3_11_11.png

 

 

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