Aktuelle Version vom 16. September 2010, 23:16 Uhr

p^{μ} = m \frac{d x^{μ}}{d τ} = γ m (\begin{matrix} c & v^{1} & v^{2} & v^{3} \end{matrix}) = (\begin{matrix} \frac{E}{c} & p^{i} \end{matrix})

p^{μ} p_{μ} = m^{2} c^{2}

Operator

\hat{p} = \frac{ℏ}{i} \underline{\nabla}

@@ Zeile 1: / Zeile 1: @@
-<math>\underline p = {\color{Grey}\hbar} \underline k</math>
+<math>\underline p = {\color{Gray} \hbar} \underline k</math>
+:<math>{{p}^{\mu }}=m\frac{d{{x}^{\mu }}}{d\tau }=\gamma m\left( \begin{matrix}
+   c & {{v}^{1}} & {{v}^{2}} & {{v}^{3}}  \\
+\end{matrix} \right)=\left( \begin{matrix}
+   \frac{E}{c} & {{p}^{i}}  \\
+\end{matrix} \right)</math>
+:<math>{{p}^{\mu }}{{p}_{\mu }}={{m}^{2}}{{c}^{2}}</math>
+=Operator=
+:<math>\hat{p}=\frac{\hbar }{\mathfrak{i}}\underline{\nabla }</math>
+[[Kategorie:Theoretische Physik]]