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Diffstat (limited to 'source/know/concept/salt-equation/index.md')
| -rw-r--r-- | source/know/concept/salt-equation/index.md | 4 |
1 files changed, 2 insertions, 2 deletions
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 $$D_0$$. |