High-energy amplitudes in N=4 SYM in the next-to-leading order

Details High-energy amplitudes in N=4 SYM in the next-to-leading order High-energy amplitudes in N=4 SYM in the next-to-leading order

2009-11-27

arxiv.org/abs/0911.5192v1

Int.J.Mod.Phys.A25:401-410,2010; Phys.Lett.B687:204-213,2010

Physics

High Energy Physics

High Energy Physics - Phenomenology

10 pages, 3 figures

Scientific paper

10.1142/S0217751X10048706 10.101

The high-energy behavior of the N=4 SYM amplitudes in the Regge limit can be calculated order by order in perturbation theory using the high-energy operator expansion in Wilson lines. At large $N_c$, a typical four-point amplitude is determined by a single BFKL pomeron. The conformal structure of the four-point amplitude is fixed in terms of two functions: pomeron intercept and the coefficient function in front of the pomeron (the product of two residues). The pomeron intercept is universal while the coefficient function depends on the correlator in question. The intercept is known in the first two orders in coupling constant: BFKL intercept and NLO BFKL intercept calculated in Ref. 1. As an example of using the Wilson-line OPE, we calculate the coefficient function in front of the pomeron for the correlator of four $Z^2$ currents in the first two orders in perturbation theory.

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