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authorPrefetch2023-02-27 15:03:21 +0100
committerPrefetch2023-02-27 15:03:21 +0100
commit52ff45a7c687d502492be0fa6e54f9b99d501465 (patch)
tree202222770fe18577ba81ce6cea146e513dfe82fa /source/know
parent75636ed8772512bdf38e3dec431888837eaddc5d (diff)
Publish "Website adventures" part 4 about images
Diffstat (limited to 'source/know')
-rw-r--r--source/know/concept/modulational-instability/index.md2
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 $$\beta_2 > 0$$.