The solution to the non–forward BFKL equation in the Leading Logarithmic approximation is expressed in terms of a sum of iterations of its kernel directly in transverse momentum and rapidity space. Several studies of the non–forward solution are performed both at the level of the gluon Green’s function and for a toy cross–section, including an analysis of the diffusion properties as found in this approach. The method developed in this paper allows for a direct inspection of the momenta in the BFKL ladder, and can be applied to solving the non–forward BFKL equation to next–to–leading logarithmic accuracy, when the corresponding kernel is available
We propose a modified Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation for the summation of large ln(l/...
The low x limit of deep inelastic electron proton scattering is considered using methods of perturba...
We suggest a modified form of a unitarized BFKL equation imposing the so-called kinematic constraint...
We propose a regularization of the BFKL equation which allows for its solution in each order of pert...
The diffractive process #gamma#p#->#V+X (where V is a vector meson and X results from the dissoci...
The high energy limit of scattering processes in QCD is, at least on the purely theoretical level, d...
The high energy limit of scattering processes in QCD is, at least on the purely theoretical level, d...
AbstractThe kernel of the BFKL equation for non-zero momentum transfer is found at next-to-leading o...
We study some analytic properties of the BFKL ladder at next-to-leading logarithmic accuracy (NLLA)....
We present approximations of varying degree of sophistication to the integral equations for the (glu...
Details of the calculation of the non-forward BFKL kernel at next-to-leading order (NLO) are offered...
We determine an approximate expression for the O(alpha(3)(S)) contribution chi(2) to the kernel of t...
In this paper we investigate the effect of introducing transverse momentum cutoffs on the BFKL equat...
Electroproduction in deep inelastic scattering at HERA is studied in a model considering a finite su...
We calculate the leading order BFKL amplitude for the exclusive diffractive process \gamma*_L(Q12) ...
We propose a modified Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation for the summation of large ln(l/...
The low x limit of deep inelastic electron proton scattering is considered using methods of perturba...
We suggest a modified form of a unitarized BFKL equation imposing the so-called kinematic constraint...
We propose a regularization of the BFKL equation which allows for its solution in each order of pert...
The diffractive process #gamma#p#->#V+X (where V is a vector meson and X results from the dissoci...
The high energy limit of scattering processes in QCD is, at least on the purely theoretical level, d...
The high energy limit of scattering processes in QCD is, at least on the purely theoretical level, d...
AbstractThe kernel of the BFKL equation for non-zero momentum transfer is found at next-to-leading o...
We study some analytic properties of the BFKL ladder at next-to-leading logarithmic accuracy (NLLA)....
We present approximations of varying degree of sophistication to the integral equations for the (glu...
Details of the calculation of the non-forward BFKL kernel at next-to-leading order (NLO) are offered...
We determine an approximate expression for the O(alpha(3)(S)) contribution chi(2) to the kernel of t...
In this paper we investigate the effect of introducing transverse momentum cutoffs on the BFKL equat...
Electroproduction in deep inelastic scattering at HERA is studied in a model considering a finite su...
We calculate the leading order BFKL amplitude for the exclusive diffractive process \gamma*_L(Q12) ...
We propose a modified Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation for the summation of large ln(l/...
The low x limit of deep inelastic electron proton scattering is considered using methods of perturba...
We suggest a modified form of a unitarized BFKL equation imposing the so-called kinematic constraint...