This commit is contained in:
hiro98 2020-06-28 20:08:58 +02:00
parent 68f18e30d0
commit 1f37fd0c1e

View file

@ -185,7 +185,7 @@ labelformat=brace, position=top]{subcaption}
\pnote{Why usefult for ev. gen -> later} \pnote{Why usefult for ev. gen -> later}
\end{frame} \end{frame}
\section{Calculation of the \(\qqgg\) Cross Section} \section{The \(\qqgg\) Cross Section}
\subsection{Approach} \subsection{Approach}
\begin{frame} \begin{frame}
\begin{figure}[ht] \begin{figure}[ht]
@ -350,6 +350,7 @@ labelformat=brace, position=top]{subcaption}
\textcolor<.->{blue}{\rho(\vb{x})} \textcolor<+->{blue}{\dd{\vb{x}}} \approx \frac{1}{N - 1}\sum_i \qty[I - \textcolor<.->{blue}{\rho(\vb{x})} \textcolor<+->{blue}{\dd{\vb{x}}} \approx \frac{1}{N - 1}\sum_i \qty[I -
\frac{f(\vb{x_i})}{\rho(\vb{x_i})}]^2 \label{eq:varI-approx} \frac{f(\vb{x_i})}{\rho(\vb{x_i})}]^2 \label{eq:varI-approx}
\end{align} \end{align}
\item<+-> No mention of dimensionality :)
\end{itemize} \end{itemize}
\end{frame} \end{frame}
@ -512,7 +513,7 @@ labelformat=brace, position=top]{subcaption}
\begin{column}{.6\textwidth} \begin{column}{.6\textwidth}
\begin{block}{Basic Idea} \begin{block}{Basic Idea}
\begin{itemize} \begin{itemize}
\item subdivide sampling volume \(\Omega\) into \(K\) \item subdivide sampling volume \(\Omega\) into
subvolumes \(\Omega_i\) subvolumes \(\Omega_i\)
\item let \(A_i = \int_{\Omega_i}f(x)\dd{x}\) \item let \(A_i = \int_{\Omega_i}f(x)\dd{x}\)
\item take \(N_i=\frac{A_i}{\sum_jA_j} \cdot N\) samples in \item take \(N_i=\frac{A_i}{\sum_jA_j} \cdot N\) samples in
@ -667,7 +668,6 @@ labelformat=brace, position=top]{subcaption}
\item intrinsic \(\pt\) \item intrinsic \(\pt\)
\item parton showers \pnote{NLO effects} \item parton showers \pnote{NLO effects}
\item hadronization \item hadronization
\item (NLO matrix elements)
\item multiple interactions \item multiple interactions
\end{itemize} \end{itemize}
\pause \(\implies\) \sherpa\ can model those effects \pause \(\implies\) \sherpa\ can model those effects