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Fragmentation of ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ in jets in pp collisions at $\sqrt{s} = 5.02~\mathrm{TeV}$
The fragmentation of jets containing a ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ meson is studied in 5.02~TeV pp data using an integrated luminosity of ${\cal L} = 27.39~\mathrm{pb^{-1}}$. The fraction of the jet transverse momentum $p_{\rm T,jet}$ carried by the ${\rm J}\hspace{-.08em}/\hspace{-...
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Lenguaje: | eng |
Publicado: |
2018
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nuclphysa.2018.09.049 http://cds.cern.ch/record/2630635 |
Sumario: | The fragmentation of jets containing a ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ meson is studied in 5.02~TeV pp data using an integrated luminosity of ${\cal L} = 27.39~\mathrm{pb^{-1}}$. The fraction of the jet transverse momentum $p_{\rm T,jet}$ carried by the ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ is measured for prompt ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ and ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ coming from b hadron decays, named nonprompt. Whereas the fragmentation function of nonprompt ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ is well-modeled by simulations using a Monte Carlo generator, the prompt ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$ are found to be accompanied by a larger level of jet activity. The fraction of \Jpsi mesons that are produced inside a jet is also reported, and found to be larger in data than in simulation, for both prompt and nonprompt ${\rm J}\hspace{-.08em}/\hspace{-.14em}\psi$. |
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