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author | Eugeniy Mikhailov <evgmik@gmail.com> | 2013-08-30 13:56:25 -0400 |
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committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2013-08-30 13:56:25 -0400 |
commit | 45b66c18d44ff1213025acd338c565c99b95e089 (patch) | |
tree | 30a61c7fa6682cc144f66d6e7c2a20b2ae59a9a3 /manual/chapters | |
parent | cfe8f5ad0050ee80d0b71e521b7be9c93d08e7b8 (diff) | |
download | manual_for_Experimental_Atomic_Physics-45b66c18d44ff1213025acd338c565c99b95e089.tar.gz manual_for_Experimental_Atomic_Physics-45b66c18d44ff1213025acd338c565c99b95e089.zip |
comma moved
Diffstat (limited to 'manual/chapters')
-rw-r--r-- | manual/chapters/interferometry.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/manual/chapters/interferometry.tex b/manual/chapters/interferometry.tex index 6e78302..bc85141 100644 --- a/manual/chapters/interferometry.tex +++ b/manual/chapters/interferometry.tex @@ -76,7 +76,7 @@ similar to that used for the Michelson interferometer, you can show that: \delta = 2d\cos\theta \end{equation}%eq.2 If this path difference produces -constructive interference, then $\delta$ is some integer multiple of , $\lambda$ namely, +constructive interference, then $\delta$ is some integer multiple of $\lambda$, namely, \begin{equation} m\lambda = 2d\cos\theta %eq.3 \end{equation}%eq.3 |