\( \newcommand{\dd}{\mathrm{d}} \) \(
\DeclareMathOperator{\sign}{sign} \) \(
\newcommand{\pvec}[1]{\vec{#1}^{\,\prime}} \) \(
\newcommand{\R}{\mathbb{R}} \)

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Special
topics in heavy-ion collision dynamics
(Transport and Magnetohydrodynamics Meeting)
\begin{equation*} p^{\mu} \frac{\partial f}{\partial x^{\mu}} + m
\frac{\partial(K^{\mu} f)}{\partial p^{\mu}} = \frac{1}{2}
\frac{g}{(2 \pi \hbar)^3} \int_{\R^3} \frac{\dd^3 \vec{p}_2}{E_2}
\int_{\R^3} \frac{\dd^3 \pvec{p}_1}{E_1'} \int_{\R^3} \frac{\dd^3
\pvec{p}_2}{E_2'} W(p_1',p_2' \leftarrow p_1,p_2) \left (f_1' f_2'
\, \overline{f} \, \overline{f}_2 - f f_1 \overline{f}_1'
\overline{f}_2' \right ) \end{equation*}
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