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Tue Sep 14 04:14:25 2010, Dmass, Misc, Doubling, Doubling results summary
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Wed Sep 15 17:04:36 2010, Dmass, Misc, Doubling, DON'T REMOVE OPTICS YET
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Wed Sep 15 22:59:37 2010, Frank, Misc, Doubling, DON'T REMOVE OPTICS YET
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Tue Sep 21 01:52:05 2010, Dmass, Misc, Doubling, Doubling results summary
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Thu Oct 6 23:44:09 2011, Dmass, Misc, Doubling, Finishing SHG paper  
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Mon Oct 10 11:55:59 2011, Dmass, Misc, Doubling, Finishing SHG paper
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Wed Sep 22 17:16:09 2010, Dmass, Misc, Doubling, Some notes on previous bounds
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Mon Jan 24 17:17:59 2011, Dmass, Misc, Doubling, Some notes on previous bounds
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Message ID: 1074
Entry time: Tue Sep 21 01:52:05 2010
In reply to: 1053
Reply to this: 1547
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Author: |
Dmass |
Type: |
Misc |
Category: |
Doubling |
Subject: |
Doubling results summary |
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I was concerned that what I thought was fractional frequency deviation might be different from clock peoples definitions of fractional frequency stability. I looked around a bit and here is what I found out:
References:
I used this to make some plots of the Allan Deviation from my power spectra, the units of Allan Deviation are dimensionless, as its a measure of fractional instability.
I found a typo in the old code, uploaded new plot.
Line / X's are calculated from the PSDs.
Circles are directly calculated Allan Deviations.
Moral: LOOKS GOOD! |
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