\begin{equation*}
\psi(\omega) = \left.{\psi}\right|_{\omega=0} +
\omega \cdot
\underbrace {\left.\dfrac{d\psi}{d\omega}\right|_{\omega=0} }_{\left.\frac{\partial \psi}{\partial x}\right|_{\substack{{x =0} \\ {y=0}}}} \,+ \,\dfrac{\omega^2}{2} \,\cdot\, \underbrace {\left.\dfrac{d^2\psi}{d\omega \, d\omega}\right|_{\substack{\omega=0}}}_{\left.\frac{\partial \psi^2}{\partial x \partial x}\right|_{\substack{x=0 \\ y=0 }}} + \ldots +
\dfrac{\omega^p}{p!} \cdot \dfrac{d^p\psi}{d\omega \cdot \ldots \cdot d\omega}
\end{equation*}
答案1
\substack
我不会将这些指令的论点简化,而是增加相关分数表达式的大小,通过使用\tfrac
而不是\frac
。
\documentclass{article}
\usepackage{amsmath,xcolor}
\begin{document}
\textcolor{red}{Before}
\begin{equation*}
\psi(\omega) = \left.{\psi}\right|_{\omega=0} +
\omega \cdot
\underbrace {\left.\dfrac{d\psi}{d\omega}\right|_{\omega=0} }_{\left.\frac{\partial \psi}{\partial x}\right|_{\substack{{x =0} \\ {y=0}}}} \,+ \,\dfrac{\omega^2}{2} \,\cdot\, \underbrace {\left.\dfrac{d^2\psi}{d\omega \, d\omega}\right|_{\substack{\omega=0}}}_{\left.\frac{\partial \psi^2}{\partial x \partial x}\right|_{\substack{x=0 \\ y=0 }}} + \ldots +
\dfrac{\omega^p}{p!} \cdot \dfrac{d^p\psi}{d\omega \cdot \ldots \cdot d\omega}
\end{equation*}
\medskip
\textcolor{red}{After}
\begin{equation*}
\psi(\omega) = \psi\bigr|_{\omega=0} +
\omega \cdot
{\underbrace {\frac{d\psi}{d\omega}\biggr|_{\omega=0} }%
_{\tfrac{\partial\psi}{\partial x}\Bigr|_{\substack{x =0\\y=0 }}}}
+
\frac{\omega^2}{2} \cdot
{\underbrace{\frac{d^2\psi}{d\omega\,d\omega}\biggr|_{\omega=0}}%
_{\tfrac{\partial^2\psi}{\partial x\,\partial x}\Bigr|_{\substack{x=0 \\ y=0 }}}}
+ \dots +
\frac{\omega^p}{p!} \cdot
\frac{d^p\psi}{d\omega \ldots d\omega}
\end{equation*}
\end{document}
答案2
LaTeX 使用 4 种数学样式:\displaystyle
、\textstyle
和。最小的\scriptstyle
是。\scriptscriptstyle
\scriptscriptstyle
\substack
,就像subarray
环境使用一样\scriptstyle
。作为一种解决方法,强制\scriptscriptstyle
内部:
\substack{\scriptscriptstyle x =0 \\ \scriptscriptstyle y=0}