of the CMS experiment.

The main objects used in this analysis are muons and particle jets, which are briefly discussed in the following. CMS employs a particle-flow algorithm that provides a complete description of the event and identifies electrons, muons, photons, charged hadrons, and neutral hadrons. Muons are reconstructed from a global fit of hits in the MS and the ID, seeded by tracks in the muon system [@CMS-PAS-MUO-10-002]. In this analysis, we require each muon to have a minimal transverse momentum of $p_T>25$ GeV within a pseudo-rapidity range of $|\eta|<2.1$, corresponding to the single muon trigger coverage. In addition, standard quality cuts on the number of hits in the ID and the MS, the $\chi^2$ of the fit as well as on the impact parameters are applied, also following previous CMS measurements [@Chatrchyan:2014mua].

Hadronic jets are reconstructed using an anti-$k_t$ algorithm [@Cacciari:2008gp; @Cacciari:2011ma] with a radius parameter of 0.5 based on particle-flow objects [@CMS-PAS-PFT-10-001; @CMS-PAS-PFT-09-001; @Sirunyan:2017ulk], where the clustering algorithms rejects objects that are coming from a pile-up vertex. A jet area method is used to correct for the remaining pile-up contributions [@Cacciari:2007fd]. Since the four-momenta of particle-flow objects is summed, the jets can be massive, In this analyses, 