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author | Prefetch | 2024-07-17 10:01:43 +0200 |
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committer | Prefetch | 2024-07-17 10:01:43 +0200 |
commit | 075683cdf4588fe16f41d9f7b46b9720b42b2553 (patch) | |
tree | f200b341b35e9c89aa1030a2f6da94cd0e1e958b /source/know/concept/salt-equation | |
parent | c4d597e8d695eb145755464cffbf88a68fd0c88a (diff) |
Improve knowledge base
Diffstat (limited to 'source/know/concept/salt-equation')
-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 $$D_0$$. |