Reconstruct the variables:
$M_t$
$M_{\bar{t}}$
$M_{W^+}$
$M_{W^-}$ Divide all in leptonic/hadronic and particle/antiparticle decays
fit a Breit-Wigner for each histogram (this is important to understand the magnitude of the non resonant decay)
Do a wider version of the plots to see the tails
- Do the same plots for
$\eta$ and$p_T$
- Create and histogram containing all the possible
$q\bar{q}$ couples and fill it with the hadronic W decaysOptional
- Multithreaded loop over events (or implement everything using the RDataframes)
Why the gluon fusion production (90%) dominate over the quark production (10%)?
At the LHC energy the bjorken variable $x=\frac{|q|^2}{2p_{in}^{\mu} q_{\mu} } $ is small and for small X the gluon PDF is much higher than the quark PDF.
For example, at the Tevatron, the CM energy was 1TeV and ttbar production was mainly from valence quarks
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Object dictionary: Documentation for mc94X_NANO.root
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pdgId: