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Diffstat (limited to 'source/know/concept/fabry-perot-cavity/index.md')
-rw-r--r-- | source/know/concept/fabry-perot-cavity/index.md | 6 |
1 files changed, 3 insertions, 3 deletions
diff --git a/source/know/concept/fabry-perot-cavity/index.md b/source/know/concept/fabry-perot-cavity/index.md index 980fa54..6eefc6e 100644 --- a/source/know/concept/fabry-perot-cavity/index.md +++ b/source/know/concept/fabry-perot-cavity/index.md @@ -19,9 +19,8 @@ We divide the $$x$$-axis into three domains: left $$L$$, center $$C$$, and right The cavity $$C$$ has length $$\ell$$ and is centered on $$x = 0$$. Let $$n_L$$, $$n_C$$ and $$n_R$$ be the respective domains' refractive indices: -<a href="cavity.png"> -<img src="cavity.png" style="width:70%"> -</a> +{% include image.html file="sketch-full.png" width="70%" alt="Cavity structure" %} + ## Microscopic cavity @@ -129,6 +128,7 @@ $$A_1$$, $$A_2$$, $$A_3$$ or $$A_4$$ freely, and then the others are determined by $$k_m$$ and the field's continuity. + ## Macroscopic cavity Next, consider a "macroscopic" Fabry-PĂ©rot cavity |