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. 2013 Aug 3;73(8):2509. doi: 10.1140/epjc/s10052-013-2509-4

Fig. 14.

Fig. 14

Ratio of the inclusive jet cross-section at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\sqrt {s}=2.76~\mbox{TeV}$\end{document} to the one at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\sqrt{s}=7~\mbox{TeV}$\end{document} as a function of x T in bins of jet rapidity, for anti-k t jets with R=0.6. The theoretical prediction is calculated at next-to-leading order with the CT10 PDF set and corrected for non-perturbative effects. Statistically insignificant data points at large x T are omitted. The 4.3 % uncertainty from the luminosity measurements is not shown