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author | Prefetch | 2022-01-30 11:27:00 +0100 |
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committer | Prefetch | 2022-01-30 11:27:00 +0100 |
commit | 88537b82784f71104c3a2771330c9e492f57fb03 (patch) | |
tree | 0d5ddb6adaf9e55892f4e7b79adf1e22cf0aee10 /content/know/concept/drude-model/index.pdc | |
parent | 8a9fb5fef2a97af3274290e512816e1a4cac0c02 (diff) |
Expand knowledge base, remove comments
Diffstat (limited to 'content/know/concept/drude-model/index.pdc')
-rw-r--r-- | content/know/concept/drude-model/index.pdc | 2 |
1 files changed, 0 insertions, 2 deletions
diff --git a/content/know/concept/drude-model/index.pdc b/content/know/concept/drude-model/index.pdc index a738dff..703ddbb 100644 --- a/content/know/concept/drude-model/index.pdc +++ b/content/know/concept/drude-model/index.pdc @@ -74,7 +74,6 @@ which depends on $\omega$: $$\begin{aligned} \boxed{ \varepsilon_r(\omega) - %= 1 - \frac{N q^2}{\varepsilon_0 m} \frac{1}{\omega^2 + i \gamma \omega} = 1 - \frac{\omega_p^2}{\omega^2 + i \gamma \omega} } \end{aligned}$$ @@ -190,7 +189,6 @@ The dielectric function $\varepsilon_r(\omega)$ is therefore given by: $$\begin{aligned} \boxed{ \varepsilon_r(\omega) - %= \varepsilon_{\mathrm{int}}(\omega) - \frac{N q^2}{\varepsilon_0 m^*} \frac{1}{\omega^2 + i \gamma \omega} = \varepsilon_{\mathrm{int}} \Big( 1 - \frac{\omega_p^2}{\omega^2 + i \gamma \omega} \Big) } \end{aligned}$$ |