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Abstract
| The relative production of the excited bottomonium states, $\Upsilon$(2S) and $\Upsilon$(3S), with respect to the ground state $\Upsilon$(1S) is measured via the dimuon decay channel in proton-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}} =$ 8.16 TeV. The analysis is based on data collected in 2016 with the CMS detector at the LHC, corresponding to an integrated luminosity of $175\,\text{nb}^{-1}$. The measurements are performed as functions of event activity, characterized by the charged-particle multiplicity measured within the pseudorapidity range $|\eta| < 2.4$, as well as the total transverse energy deposited in the forward region $4.0 < |\eta| < 5.2$. A decreasing behavior of the excited-state to ground-state yield ratios is observed with increasing charged-particle multiplicity and forward transverse energy. The measurements are compared with theoretical predictions that consider interactions of bottomonium states either with nearby particles produced in the same collision or with a hot medium that may form during the system evolution. The results provide new constraints on models describing the hadronization and modification of heavy quarks in nuclear collisions. |