From 075683cdf4588fe16f41d9f7b46b9720b42b2553 Mon Sep 17 00:00:00 2001
From: Prefetch
Date: Wed, 17 Jul 2024 10:01:43 +0200
Subject: Improve knowledge base

---
 source/know/concept/salt-equation/index.md | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'source/know/concept/salt-equation/index.md')

diff --git a/source/know/concept/salt-equation/index.md b/source/know/concept/salt-equation/index.md
index d7f8ef3..d47383f 100644
--- a/source/know/concept/salt-equation/index.md
+++ b/source/know/concept/salt-equation/index.md
@@ -275,10 +275,10 @@ so there are multiple active modes competing for charge carriers.
 
 Below threshold (i.e. before any mode is lasing), the problem is linear in $$\Psi_n$$,
 but above threshold it is nonlinear via $$h(\vb{x})$$.
-Then the amplitude of $$\Psi_n$$ gets adjusted
+Then the amplitude of $$\Psi_n$$ adjusts itself
 such that its respective $$k_n$$ never leaves the real axis.
 Once a mode is lasing, hole burning makes it harder for any other modes to activate,
-since they modes must compete for the carrier supply $$D_0$$.
+since they must compete for the carrier supply $$D_0$$.
 
 
 
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