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| author | Prefetch | 2022-03-31 21:27:48 +0200 |
|---|---|---|
| committer | Prefetch | 2022-03-31 21:27:48 +0200 |
| commit | a77d159d6a7f73252308459fe121a28df99b6df2 (patch) | |
| tree | 9fe8083659ee51dd9ff898dcd9f07ec198fb15b8 /content/know/concept/salt-equation | |
| parent | eacd6f7bc1a4a048e1352b740dd3354e2a035106 (diff) | |
Expand knowledge base
Diffstat (limited to 'content/know/concept/salt-equation')
| -rw-r--r-- | content/know/concept/salt-equation/index.pdc | 5 |
1 files changed, 3 insertions, 2 deletions
diff --git a/content/know/concept/salt-equation/index.pdc b/content/know/concept/salt-equation/index.pdc index 2f2917b..6383469 100644 --- a/content/know/concept/salt-equation/index.pdc +++ b/content/know/concept/salt-equation/index.pdc @@ -5,6 +5,7 @@ publishDate: 2022-02-07 categories: - Physics - Optics +- Laser theory date: 2022-01-20T22:01:48+01:00 draft: false @@ -66,10 +67,10 @@ that the interactions between the modes are limited: $$\begin{aligned} \vb{E}^{+}(\vb{x}, t) - = \sum_{n = 1}^N \Psi_n(\vb{x}) e^{- i \omega_n t} + = \sum_{n = 1}^N \Psi_n(\vb{x}) \: e^{- i \omega_n t} \qquad \qquad \vb{P}^{+}(\vb{x}, t) - = \sum_{n = 1}^N \vb{p}_n(\vb{x}) e^{- i \omega_n t} + = \sum_{n = 1}^N \vb{p}_n(\vb{x}) \: e^{- i \omega_n t} \end{aligned}$$ Using the modes' linear independence to treat each term of the summation individually, |