\documentclass[10pt]{beamer}
\usetheme[progressbar=frametitle]{metropolis}
\usepackage[english]{babel}
\usepackage{booktabs}
\usefonttheme[onlymath]{serif}
\setbeamercolor{background canvas}{bg=white}
\setbeamertemplate{footline}[frame number]
\usetheme{Singapore}
\usepackage{xcolor}
\begin{document}
\begin{frame}{Standard Model}
Standard Model(SM) is gauge theory based on the gauge group-
\begin{equation}
G_{SM}= SU(3)_C\times SU(2)_L\times U(1)_Y
\end{equation}
Complete SM lagrangian can be written as-
\[\mathcal{L}_{SM}=\textcolor{blue}{i\overline{\psi}\gamma^{\mu}\mathcal{D}_{\mu}\psi}\pause\textcolor{red}{ -\frac{1}{4}G^{\mu\nu A}G_{\mu\nu}^{A}-\frac{1}{4}W^{\mu\nu I}W_{\mu\nu}^{I}-\frac{1}{4}B^{\mu\nu}B_{\mu\nu}}\]
\[\pause\textcolor{magenta}{+h_{ij}^{u}\overline{Q}_{i}U_{j} \widetilde{H}+h_{ij}^{d}\overline{Q}_{i} D_{j}H+h_{ij}^{e}\overline{L}_{i}E_{j}H+h.c.}\]
\pause
\begin{equation}
\textcolor{violet}{+(\mathcal{D}_{\mu}H)^{\dag}\mathcal{D}_{\mu}H-\mu^{2}H^{\dag}H+\lambda(H^{\dag}H)^{2}}
\end{equation}
\end{frame}
\end{document}
我希望这些幻灯片中包含每个术语的框式描述,但当我跳转到下一个术语或下一张幻灯片时,前一个描述应该消失。我该如何实现?
答案1
如果您只想在一张幻灯片中添加文本,请尝试\only<>{}
\documentclass{beamer}
\begin{document}
\begin{frame}
Complete SM lagrangian can be written as-
\[\mathcal{L}_{SM}=\textcolor{blue}{i\overline{\psi}\gamma^{\mu}\mathcal{D}_{\mu}\psi}\only<1>{~\fbox{explain something}}\pause
\textcolor{red}{ -\frac{1}{4}G^{\mu\nu A}G_{\mu\nu}^{A}-\frac{1}{4}W^{\mu\nu I}W_{\mu\nu}^{I}-\frac{1}{4}B^{\mu\nu}B_{\mu\nu}}\]
\[\pause\textcolor{magenta}{+h_{ij}^{u}\overline{Q}_{i}U_{j} \widetilde{H}+h_{ij}^{d}\overline{Q}_{i} D_{j}H+h_{ij}^{e}\overline{L}_{i}E_{j}H+h.c.}\]
\pause
\begin{equation}
\textcolor{violet}{+(\mathcal{D}_{\mu}H)^{\dag}\mathcal{D}_{\mu}H-\mu^{2}H^{\dag}H+\lambda(H^{\dag}H)^{2}}
\end{equation}
\end{frame}
\end{document}
在https://tex.stackexchange.com/a/205623/36296你也可以像这样解释术语
\documentclass{beamer}
\usepackage{mathtools}
\newcommand<>{\uncoverubrace}[2]{%
\onslide#3 \underbrace{ \onslide<1->%
#1%
\onslide#3 }_{#2} \onslide<1->%
}
\newcommand<>{\uncoverobrace}[2]{%
\onslide#3 \overbrace{ \onslide<1->%
#1%
\onslide#3 }^{#2} \onslide<1->%
}
\begin{document}
\begin{frame}
Complete SM lagrangian can be written as-
\[\mathcal{L}_{SM}=\uncoverubrace<1>{\textcolor{blue}{i\overline{\psi}\gamma^{\mu}\mathcal{D}_{\mu}\psi}}{\only<1>{\fbox{matter}}}\pause
\textcolor{red}{ -\frac{1}{4}G^{\mu\nu A}G_{\mu\nu}^{A}-\frac{1}{4}W^{\mu\nu I}W_{\mu\nu}^{I}-\frac{1}{4}B^{\mu\nu}B_{\mu\nu}}\]
\[\pause\textcolor{magenta}{+h_{ij}^{u}\overline{Q}_{i}U_{j} \widetilde{H}+h_{ij}^{d}\overline{Q}_{i} D_{j}H+h_{ij}^{e}\overline{L}_{i}E_{j}H+h.c.}\]
\pause
\begin{equation}
\textcolor{violet}{+(\mathcal{D}_{\mu}H)^{\dag}\mathcal{D}_{\mu}H-\mu^{2}H^{\dag}H+\lambda(H^{\dag}H)^{2}}
\end{equation}
\end{frame}
\end{document}