We perform a precise calculation of the transverse momentum ( q T ) distribution of the boson+jet system in boson production events. The boson can be either a photon, W , Z or Higgs boson with mass m V , and q T is the sum of the transverse momenta of the boson and the leading jet with magnitude q T = | q T |. Using renormalization group techniques and soft-collinear effective theory, we resum logarithms log(Q/q T ) and log R at next-to-leading logarithmic accuracy including the non-global logarithms, where Q and R are respectively the hard scattering energy and the radius of the jet. Specifically, we investigate two scenarios of p J T m V or p J T m V in Z+jet events, and we examine the q T distributions with different jet radii and study the effect of non-global logarithms. In the end we compare our theoretical calculations with Monte Carlo simulations and data from the LHC.
A The Hard Function at LO 26 B Anomalous Dimensions 27 C LO singular terms 28-1 -1 Recently, much progress was made in the study of NGL resummation [29][30][31][32][33][34][35][36][37][38][39][40][41][42][43][44].where we have neglected the dependence of the jet function on n 1 · x and n 2 · x, which will be justified in the next subsection. Likewise, P α J α J n J is the projector defined as expanding the integrand around p 2 J = 0 in (2.17) gives ∞ 0 dp 2 J δ(n J · p J − m i=1 n J · p J i ) =n J · p J .(2.20)