Abstract

We derive a factorization theorem for the jet mass distribution with a given $$p_T^J$$ for the inclusive production, where $$p_T^J$$ is a large jet transverse momentum. Considering the small jet radius limit (R ≪ 1), we factorize the scattering cross section into a partonic cross section, the fragmentation function to a jet, and the jet mass distribution function. The decoupled jet mass distributions for quark and gluon jets are well-normalized and scale invariant, and they can be extracted from the ratio of two scattering cross sections such as $$d\sigma/(dp_T^JdM_J^2)$$ and $$d\sigma/dp_T^J$$ . When $$M_J \sim p_T^JR$$ , the perturbative series expansion for the jet mass distributions works well. As the jet mass becomes small, large logarithms of $$M_J/(p_T^JR)$$ appear, and they can be systematically resummed through a more refined factorization theorem for the jet mass distribution.

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