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| author | Prefetch | 2021-05-28 15:27:37 +0200 |
|---|---|---|
| committer | Prefetch | 2021-05-28 15:27:37 +0200 |
| commit | 9657833b115c8a61509295d2296c6f89e81fd219 (patch) | |
| tree | 957ac6c1eb897c13939d849513508145d7d258f7 /content/know/concept/dispersive-broadening/index.pdc | |
| parent | 4780106a4f191c41d3b82ca9d1327a1c95a72055 (diff) | |
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Diffstat (limited to 'content/know/concept/dispersive-broadening/index.pdc')
| -rw-r--r-- | content/know/concept/dispersive-broadening/index.pdc | 7 |
1 files changed, 7 insertions, 0 deletions
diff --git a/content/know/concept/dispersive-broadening/index.pdc b/content/know/concept/dispersive-broadening/index.pdc index f053eb6..cae856d 100644 --- a/content/know/concept/dispersive-broadening/index.pdc +++ b/content/know/concept/dispersive-broadening/index.pdc @@ -93,3 +93,10 @@ Of great importance is the sign of $\beta_2$: in the **anomalous dispersion regime** ($\beta_2 < 0$), lower frequencies travel more slowly than higher ones, and vice versa in the **normal dispersion regime** ($\beta_2 > 0$). + + + +## References +1. O. Bang, + *Numerical methods in photonics: lecture notes*, 2019, + unpublished. |