summaryrefslogtreecommitdiff
path: root/source/know/concept/drude-model
diff options
context:
space:
mode:
authorPrefetch2023-06-18 17:59:42 +0200
committerPrefetch2023-06-18 17:59:42 +0200
commite2f6ff4487606f4052b9c912b9faa2c8d8f1ca10 (patch)
tree16455ba80b2ff443a970945a7ca8bd49cfc8377b /source/know/concept/drude-model
parent5a4eb1d13110048b3714754817b3f38d7a55970b (diff)
Improve knowledge base
Diffstat (limited to 'source/know/concept/drude-model')
-rw-r--r--source/know/concept/drude-model/index.md6
1 files changed, 3 insertions, 3 deletions
diff --git a/source/know/concept/drude-model/index.md b/source/know/concept/drude-model/index.md
index c4faf81..0026d90 100644
--- a/source/know/concept/drude-model/index.md
+++ b/source/know/concept/drude-model/index.md
@@ -11,7 +11,7 @@ layout: "concept"
The **Drude model**, also known as
the **Drude-Lorentz model** due to its analogy
-to the *Lorentz oscillator model*
+to the [Lorentz oscillator model](/know/concept/lorentz-oscillator-model/)
classically predicts the [dielectric function](/know/concept/dielectric-function/)
and electric conductivity of a gas of free charges,
as found in metals and doped semiconductors.
@@ -59,7 +59,7 @@ $$\begin{aligned}
= - \frac{N q^2}{m (\omega^2 + i \gamma \omega)} \vb{E}(t)
\end{aligned}$$
-The electric displacement field $$\vb{D}$$ is then as follows,
+The electric displacement field $$\vb{D}(t)$$ is then as follows,
where the parenthesized expression is the dielectric function
$$\varepsilon_r$$ of the material:
@@ -180,7 +180,7 @@ We must replace the carriers' true mass $$m$$ with their *effective mass* $$m^*$
found from the material's electronic band structure.
Furthermore, semiconductors already have
a high intrinsic dielectric function $$\varepsilon_{\mathrm{int}}$$
-before being doped, so the displacement field $$\vb{D}$$ becomes:
+before being doped, so the displacement field $$\vb{D}(t)$$ becomes:
$$\begin{aligned}
\vb{D}