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| author | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-09-05 08:54:12 -0400 |
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| committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-09-05 08:54:12 -0400 |
| commit | 2facdf6a316829750773dda05b72fbcccd1b139c (patch) | |
| tree | fe4c0afe2a75998506d5df2b4764a1f39bd28209 | |
| parent | 5e32fa95cec1734ebe84ca60d627e49c705cb555 (diff) | |
| download | manual_for_Experimental_Atomic_Physics-2facdf6a316829750773dda05b72fbcccd1b139c.tar.gz manual_for_Experimental_Atomic_Physics-2facdf6a316829750773dda05b72fbcccd1b139c.zip | |
typo fix, thanks Michael
| -rw-r--r-- | interferometry.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/interferometry.tex b/interferometry.tex index ef14794..02c1b3d 100644 --- a/interferometry.tex +++ b/interferometry.tex @@ -56,7 +56,7 @@ In \textbf{Fabry-Perot configuration} the input light field bounces between two A Fabry-Perot interferometer consists of two parallel glass plates, flat to better than 1/4 of an optical wavelength $\lambda$, and coated on the inner surfaces with a partially transmitting metallic layer. Such two-mirror arrangement is normally called an {\it optical cavity}. The light in a cavity by definition bounces -back and forth many time before escaping; the idea of such a cavity is crucial for the construction of a laser. +back and forth many times before escaping; the idea of such a cavity is crucial for the construction of a laser. Any light transmitted through such cavity is a product of interference between beams transmitted at each bounce as diagrammed in Figure~\ref{fpfig1}. When the incident ray arrives at interface point $A$, a fraction $t$ is transmitted and the remaining fraction $r$ is reflected, such that $t + r = 1$ ( this assumes no light is lost |