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| author | Prefetch | 2023-02-27 15:03:21 +0100 |
|---|---|---|
| committer | Prefetch | 2023-02-27 15:03:21 +0100 |
| commit | 52ff45a7c687d502492be0fa6e54f9b99d501465 (patch) | |
| tree | 202222770fe18577ba81ce6cea146e513dfe82fa /source/know/concept/modulational-instability | |
| parent | 75636ed8772512bdf38e3dec431888837eaddc5d (diff) | |
Publish "Website adventures" part 4 about images
Diffstat (limited to 'source/know/concept/modulational-instability')
| -rw-r--r-- | source/know/concept/modulational-instability/index.md | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/source/know/concept/modulational-instability/index.md b/source/know/concept/modulational-instability/index.md index d646503..3c0de4b 100644 --- a/source/know/concept/modulational-instability/index.md +++ b/source/know/concept/modulational-instability/index.md @@ -198,7 +198,7 @@ then it can in turn also cause MI in its own surroundings, leading to a cascade of secondary and tertiary gain areas. This is seen above for $$z > 30 L_\mathrm{NL}$$. -What we described is "pure" MI, but there also exists +Here we described "pure" MI, but there also exists a different type caused by Raman scattering. In that case, amplification occurs at the strongest peak of the Raman gain $$\tilde{g}_R(\omega)$$, even when the parent pulse has $$\beta_2 > 0$$. |