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Angular structure of jet quenching within a hybrid strong/weak coupling model

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Academic year: 2021

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Figure 2. Dependence of R jet AA on the anti-k t jet reconstruction parameter R for K = 0 (no broadening, left panel) and K = 40 (right panel)
Figure 3. Dijet acoplanarity distribution for high-energy (left) and low-energy (right) dijets in LHC heavy ion collisions with √ s = 2.76 ATeV for two different values of the broadening parameter K
Figure 4. Dijet acoplanarity distribution for dijets in heavy ion collisions at RHIC for different values of the broadening parameter K
Figure 5. Left: ratio of the jet shape in PbPb collisions to that in proton-proton collisions for different values of the broadening parameter K as compared to CMS data from heavy ion collisions with √ s = 2.76 ATeV [51] and 0-10% centrality (left) or 10-3
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