1-loop matching and NNLL resummation for all partonic 2 to 2 processes in QCD

Details 1-loop matching and NNLL resummation for all partonic 2 to 2 processes in QCD 1-loop matching and NNLL resummation for all partonic 2 to 2 processes in QCD

2010-08-16

arxiv.org/abs/1008.2759v2

Phys.Rev.D83:045022,2011

Physics

High Energy Physics

High Energy Physics - Phenomenology

28 pages, 5 tables; v2: typo corrected in Eq. (56)

Scientific paper

10.1103/PhysRevD.83.045022

The Wilson Coefficients for all 4-parton operators which arise in matching QCD to Soft-Collinear Effective Theory (SCET) are computed at 1-loop. Any dijet observable calculated in SCET beyond leading order will require these results. The Wilson coefficients are separated by spin and color, although most applications will involve only the spin-averaged hard functions. The anomalous dimensions for the Wilson coefficients are given to 2-loop order, and the renormalization group equations are solved explicitly. This will allow for analytical resummation of dijet observables to next-to-next-to-leading logarithmic accuracy. For each channel, there is a natural basis in which the evolution is diagonal in color space. The same basis also diagonalizes the color evolution for the soft function. Even though soft functions required for SCET calculations are observable dependent, it is shown that their renormalization group evolution is almost completely determined by a universal structure. With these results, it will be possible to calculate hadronic event shapes or other dijet observables to next-to-leading order with next-to-next-to-leading log resummation.

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