Jets have long been used as an effective probe for exploring the properties of the quark-gluon plasma (QGP) produced in high energy collisions of nuclei [1]. In heavy ion collisions some nucleons will undergo hard scattering, breaking apart and releasing their constituent high transverse momentum partons. These partons undergo hadronization due to the phenomenon of colour confinement. This is a process in which, as the constituent partons separate, the strong coupling constant increases until there is enough potential energy for it to be more energetically favourable to produce a quark-antiquark pair. This radiates more partons, predominantly collinear with their parent, forming jets of particles. As the energy of these particles decrease they will form colourless hadrons which can be detected. We set out with the aim to establish a groundwork for measuring the shape of the QGP by examining the energy loss of jets with respect to the azimuthal angle. By examining Z+jet events we aim to accurately measure the jet energy lost through jet quenching in the QGP. We expect jets which have traversed a larger distance in the QGP to lose more energy and thus an azimuthal anisotropy of jet energy loss will give us information on the shape of the produced QGP. While the latest run at the LHC did not yield many Z events from PbPb collisions [2] the next run should provide the data necessary for a complete analysis of this type. We will make use of a dijet enhanced Monte Carlo (MC) dataset in order to plan out the process and collect preliminary results.

The production of jets in association with Z bosons, reconstructed via the mu+mu- and e+e- decay channels, is studied in pp and, for the first time, in PbPb collisions. Both data samples were collected by the CMS experiment at the LHC, at a center-of-mass energy of 5.02 TeV. The PbPb collisions were analyzed in the 0-30% centrality range. The back-to-back azimuthal alignment was studied in both pp and PbPb collisions for Z bosons with transverse momentum ptz> 60 GeV/c and a recoiling jet with ptj> 30 GeV/c. The pt imbalance, xjz= ptj/ptz, as well as the average number of jet partners per Z, rjz, were studied in intervals of ptz, in both pp and PbPb collisions. The rjz is found to be smaller in PbPb than in pp collisions, which suggests that in PbPb collisions a larger fraction of partons, associated with the Z bosons, lose energy and fall below the 30 GeV/c ptj threshold.

Interactions between jets and the quark-gluon plasma produced in heavy ion collisions are studied via the angular distributions of summed charged-particle transverse momenta (pT) with respect to both the leading and subleading jet axes in high-pt dijet events. The contributions of charged particles in different momentum ranges to the overall event pt balance are decomposed into short-range jet peaks and a long-range azimuthal asymmetry in charged-particle pT. The results for PbPb collisions are compared to those in pp collisions using data collected in 2011 and 2013, at collision energy $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $ TeV with integrated luminosities of 166 [mu]b-1 and 5.3 pb-1, respectively, by the CMS experiment at the LHC. Furthermore, measurements are presented as functions of PbPb collision centrality, charged-particle pt, relative azimuth, and radial distance from the jet axis for balanced and unbalanced dijets.

Jet production in PbPb collisions at a nucleon-nucleon center-of-mass energy of 2.76 TeV was studied with the CMS detector at the LHC, using a data sample corresponding to an integrated luminosity of 6.7 inverse microbarns. Jets are reconstructed using the energy deposited in the CMS calorimeters and studied as a function of collision centrality. With increasing collision centrality, a striking imbalance in dijet transverse momentum is observed, consistent with jet quenching. The observed effect extends from the lower cut-off used in this study (jet transverse momentum = 120 GeV/c) up to the statistical limit of the available data sample (jet transverse momentum approximately 210 GeV/c). Correlations of charged particle tracks with jets indicate that the momentum imbalance is accompanied by a softening of the fragmentation pattern of the second most energetic, away-side jet. The dijet momentum balance is recovered when integrating low transverse momentum particles distributed over a wide angular range relative to the direction of the away-side jet.

The aim of this study was to investigate the phenomenon of jet quenching due to the formation of the quark-gluon plasma in heavy ion and proton-proton collisions. This was done by comparing the transverse momentum, pT , ratio between a jet of hadronic particles, and a Z boson in both Monte Carlo simulations and real datasets, collected during the 2015 run of the Large Hadron Collider, using the Compact Muon Solenoid detector. The pT imbalance was studied in three di erent regions, namely for events where the Z boson had transverse momentum pT > 30GeV, pT > 60GeV and pT > 100GeV. The results show that there is a signi cant suppression of the jet pT in central heavy ion collisions compared to the proton-proton collisions, and the pT ratio decreases with higher initial pT.

In a collision experiment involving highly energetic particles such as hadrons, processes at high momentum transfers can provide information useful for many studies involving Quantum Chromodynamics (QCD). One way of analyzing these interactions is through angular distributions. In hadron-hadron collisions, the angular distribution between the two leading jets with the largest transverse momentum (pT) is affected by the production of additional jets. While soft radiation causes small differences in the azimuthal angular distribution of the two leading jets produced in a collision event, additional hard jets produced in the event have more pronounced influence on the distribution of the two leading jets produced in the collision. Thus, the dijet azimuthal angular distribution can serve as a variable that can be used to study the transition from soft to hard QCD processes in a collision event. This dissertation presents a triple-differential study involving the azimuthal angular distribution and the jet transverse momenta, and jet rapidities of the first two leading jets. The data used for this research are obtained from proton-antiproton (p$\bar{p}$) collisions occurring at a center of mass energy of 1.96TeV, using the DØ detector in Run II of the Tevatron Collider at the Fermi National Accelerator Laboratory (FNAL) in Illinois, USA. Comparisons are made to perturbative QCD (pQCD) predictions at next-to-leading order (NLO).