Figure 14

Left: The nuclear modification factor \RpPbBjet of the inclusive charged-particle anti-$k_{\rm T}$ $R=0.4$ b jets as a function of \pt from the IP and SV method. Right: The nuclear modification factor \RpPbBjet obtained from combining the IP and SV method results as a function of \pTchjet compared with the calculation by the POWHEG dijet tune with the PYTHIA 8 fragmentation  Systematic and statistical uncertainties are shown as boxes and error bars, respectively. There is an additional normalization uncertainty of $4.37\%$ due to luminosity, which is quoted separately.