Large N QCD at High Energies as Two-Dimensional Field Theory
arXiv:hep-th/9306014 · doi:10.1016/0370-2693(94)91499-0
Abstract
Different aspects of the Verlinde and Verlinde relation between high-energy effective scattering in QCD and a two-dimensional sigma-model are discussed. Starting from a lattice version of the truncated 4-dimensional Yang-Mills action we derive an effective theory with non-trivial longitudinal dynamics which has a form of the lattice two-dimensional chiral field model with non-trivial boundary conditions. To get quantum corrections coming from non-trivial longitudinal dynamics to transversal high-energy effective action one has to solve the two-dimensional chiral field model with non-trivial boundary conditions. We do this within an approximation scheme which takes into account one-dimensional excitations. Contributions of the one-dimensional excitations to quantum corrections for the high-energy effective action are calculated in the large N limit using the character expansion method.
Latex, 14pages, one reference added+ some minor corrections
References in corpus (1)
Cited by in corpus (10)
- Feynman rules for effective Regge action
- A remark on the high--energy quark--quark scattering and the eikonal approximation
- Regge Regime in QCD and Asymmetric Lattice Gauge Theory
- A nonperturbative foundation of the Euclidean-Minkowskian duality of Wilson-loop correlation functions
- Formulating Light Cone QCD on the Lattice
- Eikonal propagators and high-energy parton-parton scattering in gauge theories
- High energy scattering in Einstein-Cartan gravity
- Near-integrability and confinement for high-energy hadron-hadron collisions
- Gluon Structure Function of a Color Dipole in the Light-Cone Limit of Lattice QCD
- Renormalisation of gauge theories on general anisotropic lattices and high-energy scattering in QCD