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\chapter{Íàçâàíèå ãëàâû}
\section{Íàçâàíèå ñåêöèè}
Âíóòðèòåêñòîâàÿ ôîðìóëà $\frac{1}{\epsilon^*}=\frac{1}{\epsilon_\infty}-\frac{1}{\epsilon_0}$.
\nomenclature{$\epsilon_\infty$}{âûñîêî÷àñòîòíàÿ äèýëåêòðè÷åñêàÿ ïðîíèöàåìîñòü}
\nomenclature{$\epsilon_0$}{ñòàòè÷åñêàÿ äèýëåêòðè÷åñêàÿ ïðîíèöàåìîñòü}
Âíóòðèòåêñòîâàÿ ôîðìóëà â ñòèëå âûäåëåííîé $\dfrac{1}{\epsilon_\infty}$.
Ññûëêè íà ëèòåðàòóðó~\cite{Yoffe_1993_AP_42_173,Efros_1982_FTP_16_7_1209,%
Anselm_1978,Segall_1968,Agranovich_1983,InP,Mishchenko_1996,Skvortsov_2008,%
Perelman_2003_math:0307245,Nielsen_2010_1006.2735,patent1,patent2}.
Ññûëêà íà ôîðìóëó~\eqref{e:Coulomb}
\begin{equation}\label{e:Coulomb}
\frac{1}{|\vec r_1 - \vec r_2|} =
4\pi \int \frac{d^3 q}{(2\pi)^3}\,
\frac{e^{i\vec q(\vec r_1 - \vec r_2)}}{q^2},
\end{equation}
ãäå \nomencl{$\vec r_i$}{êîîðäèíàòà $i$-é ÷àñòèöû}.
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