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author | Blaise Thompson <blaise@untzag.com> | 2018-04-26 10:51:26 -0500 |
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committer | Blaise Thompson <blaise@untzag.com> | 2018-04-26 10:51:26 -0500 |
commit | b6d88e014f454e040a96d6f1342cefff0c99f061 (patch) | |
tree | 638602e15e9db7803ab09bfcae894807e2901dff /opa_phase | |
parent | 927603036226f1404001062b512ee6dee3c8fbc6 (diff) |
2018-04-26 10:51
Diffstat (limited to 'opa_phase')
-rw-r--r-- | opa_phase/chapter.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/opa_phase/chapter.tex b/opa_phase/chapter.tex index ae1a9ea..6fef62f 100644 --- a/opa_phase/chapter.tex +++ b/opa_phase/chapter.tex @@ -7,7 +7,7 @@ This makes interference processes quickly average to zero over many shots---we r than 100 shots per pixel. % Here I demonstrate that this assumption is very poor, at least for the femtosecond OPAs. % -In these experiments, I simply send OPA1 and OPA2 simultaniously into the array detector. % +In these experiments, I simply send OPA1 and OPA2 simultaneously into the array detector. % The crucial detail is that the beams are exactly collinear---overlaped in a beamsplitter. % I then scan delay between them while collecting single shot spectra using the array detector. % |