From 7695f5ef971de3b2c03e17aed215b8d2a8a47df5 Mon Sep 17 00:00:00 2001 From: Ana Andrade Date: Wed, 23 Oct 2024 10:25:08 +0000 Subject: [PATCH] Update on Overleaf. --- sections/goal.tex | 2 +- sections/producer.tex | 4 ++++ 2 files changed, 5 insertions(+), 1 deletion(-) diff --git a/sections/goal.tex b/sections/goal.tex index 6f4adaa..436b561 100644 --- a/sections/goal.tex +++ b/sections/goal.tex @@ -1,4 +1,4 @@ -\section{Physics example: $H \rightarrow ZZ \rightarrow 4l$} +\section{Physics example: H $\rightarrow$ ZZ $\rightarrow$ 4l} \justifying \paragraph{} The goal of this exercise is to reconstruct the standard model (SM) Higgs boson mass, using a selection targeting the four-lepton final state. This is considered a \textit{golden} channel to measure the properties of the Higgs boson because: diff --git a/sections/producer.tex b/sections/producer.tex index e9932f2..aef7728 100644 --- a/sections/producer.tex +++ b/sections/producer.tex @@ -1 +1,5 @@ \section{Writing a Producer}\label{sec:producer} + +The \CCSPStlye{Producer} class is used to calculate higher-level observables and define new columns to be written o disk. The corresponding task is called \CCSPStlye{cf.ProduceColumns} (see Ref.~\cite{cf_repo} for detailed info). Naturally, we only want to compute these new variables for the relevant events for our analysis. Thus, the producers are executed after the selection step. + +In this part of the tutorial, we will write a producer which calculates the four lepton invariant mass.