\begin{frame}{Calcolo classico}
\vspace{-1cm}
\begin{equation*}
mv = \dfrac{E_{\gamma}}{c} + m(v-v_{R}); \qquad
E_{e} + \dfrac{1}{2}mv^{2} = E_{f} + E_{\gamma} + \dfrac{1}{2}m(v-v_{R})^{2}\\
\vspace{0.1cm}
\textcolor{blue}{Ponendo:}\\
E_{R} = \dfrac{1}{2}mv_{R}^{2} = \dfrac{E_{\gamma}^{2}}{2mc^{2}} \approx \dfrac{E_{0}^{2}}{2mc^{2}}; \qquad
\vspace{0.1cm}
E_{D} = mvv_{R} = \dfrac{E_{\gamma}v}{c} \approx \dfrac{E_{0}v}{c}\\
\vspace{0.1cm}
\textcolor{blue}{ Otteniamo:}\\
E_{\gamma}= E_{0} -E_{R} +E_{D}\\
\vspace{0.3cm}
\textcolor{blue}{ Per v=0, per avere fluorescenza di risonanza si deve avere:}\\
2E_{R} \lesssim \Gamma \\ \textcolor{black}{(condizione non verificata per nuclei con E_{0}= 100KeV; A=100)}\\
\end{equation*}
\vspace{-1.5cm}
\begin{equation*}
\textcolor{blue}{Agitazione termica} \Rightarrow \delta v= \sqrt{\frac{k_{B}T}{m}} \Rightarrow \Gamma_{D} = \dfrac{E_{0}\delta v}{c}= \dfrac{E_{0}}{c}\sqrt{\frac{k_{B}T}{m}}\\ \textcolor{black}{(caso tipico nucleare \Gamma_{D}=10^{-3} eV)} \\
\end{equation*}
\end{frame}
[Tex/LaTex] missing $ inserted .\end{frame}
beamermath-mode
Best Answer
This is a combination of multiple problems:
don't leave empty lines in equations
put each equation in its own
equation*
environmentdon't abuse
\\
for line breaks, if you are in text mode, leave an empty line instead