\def\GWslide{
\begin{frame} \frametitle{Fusion Reaction}
  \begin{figure}[t]
    \centering
    \GWigwc{0.5}{Theory/Fusion/FusionIntro/FusionReaction/fig/fig}{wiki:NuclFus}
  \end{figure}
\end{frame}}

\def\GWslideCz{
\begin{frame} \frametitle{Fúzní $\rm ^2_1H$ - $\rm ^3_1H$ (deuterium - tritium) reakce\\ (nejvhodnější kandidát do pozemských podmínek)}
\centering
  \begin{figure}[t]
     \GWigwc{0.5}{Theory/Fusion/FusionIntro/FusionReaction/fig/Landscape.png}{wiki:NuclFus}
  \end{figure}
%\LARGE 
$\bf ^2_1H_{10\ keV}$ + $\bf^3_1H_{10\ keV}\Rightarrow$ $\bf^4_2He_{3.5\ MeV}$+$\bf^1_0n_{14.1\ MeV}$\\~\\
%\LARGE 
\small $m_{\rm ^2H}=2.01355m_u$, $m_{\rm ^3H}=3.01550m_u$, $m_{\rm He}=4.00150m_u$, $m_{\rm n}=1.007332m_u$\newline 
%$m_p=1.00867m_u$,
\normalsize $m_{\rm (^2H+^3H)}=5.02905 m_u$,$m_{\rm (He+n)}=5.01017 m_u$, \\ pak hmotnostn\'\i\ schodek $\Delta m$ $=0.01888 m_u$.
\small \newline $E=\Delta m\ c^2$:\  $E=\Delta m$ kr\'at $\frac{c^2m_u}{e}$=$17.6$ MeV\\~\\
$1 \rm eV\sim 11600 ^\circ C$
$\approx \ \ \bf ^2_1H_{100\ M^\circ C}$ + $\bf^3_1H_{100\ M^\circ C}\Rightarrow$ $\bf^4_2He_{35\ G^\circ C}$+$\bf^1_0n_{141\ G^\circ C}$\\
\end{frame}}