The semi-inclusive jet function in SCET and small radius resummation for inclusive jet production

A bstract We introduce a new kind of jet function: the semi-inclusive jet function J i ( z, ω J , μ ), which describes how a parton i is transformed into a jet with a jet radius R and energy fraction z = ω J /ω , with ω J and ω being the large light-cone momentum component of the jet and the corresponding parton i that initiates the jet, respectively. Within the framework of Soft Collinear Effective Theory (SCET) we calculate both J q ( z, ω J , μ ) and J g ( z, ω J , μ ) to the next-to-leading order (NLO) for cone and anti-k T algorithms. We demonstrate that the renormalization group (RG) equations for J i ( z, ω J , μ ) follow exactly the usual DGLAP evolution, which can be used to perform the ln R resummation for inclusive jet cross sections with a small jet radius R . We clarify the difference between our RG equations for J i ( z, ω J , μ ) and those for the so-called unmeasured jet functions J i ( ω J , μ ), widely used in SCET for exclusive jet production. Finally, we present applications of the new semi-inclusive jet functions to inclusive jet production in e + e − and pp collisions. We demonstrate that single inclusive jet production in these collisions shares the same short-distance hard functions as single inclusive hadron production, with only the fragmentation functions D i h ( z , μ ) replaced by J i ( z, ω J , μ ). This can facilitate more efficient higher-order analytical computations of jet cross sections. We further match our ln R resummation at both LL R and NLL R to fixed NLO results and present the phenomenological implications for single inclusive jet production at the LHC.