Abstract
We address the problem of solution of the QCD three-particle evolution equations which govern the Q(2)-dependence of the chiral-even quark-gluon-quark and three-gluon correlators contributing to a number of asymmetries at leading order and the transversely polarized structure function g(2)(x(Bj)). The quark-gluon-quark case is completely integrable in multicolour limit and corresponds to a spin ...
Abstract
We address the problem of solution of the QCD three-particle evolution equations which govern the Q(2)-dependence of the chiral-even quark-gluon-quark and three-gluon correlators contributing to a number of asymmetries at leading order and the transversely polarized structure function g(2)(x(Bj)). The quark-gluon-quark case is completely integrable in multicolour limit and corresponds to a spin chain with non-periodic boundary conditions, while the pure gluonic sector contains, apart from a piece in the Hamiltonian equivalent to XXX Heisenberg magnet of spin s = -3/2, a non-integrable addendum which can be treated perturbatively for a bull; of the spectrum except for a few lowest energy levels. We construct a quasiclassical expansion with respect to the total conformal spin of the system and describe fairly well the energy spectra of quark-gluon-quark and three-gluon systems. (C) 2000 Elsevier Science B.V. All rights reserved.
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