Abstract

It is well understood that the leading logarithmic approximation for the amplitudes of high energy processes is insufficient and that the next-to-leading logarithmic effects are very large and lead to instability of the solution. The resummation at low x, which includes kinematical constraints and other corrections leads to stable result. Using previously established resummation procedure we study in detail the preasymptotic effects which occur in the solution to the resummed BFKL equation when the energy is not very large. We find that in addition to the well known reduction of the intercept, which governs the energy dependence of the gluon Green’s function, resummation leads to the delay of the onset of its small x growth. Moreover the gluon Green’s function develops a dip or a plateau in wide range of rapidities, which increases for large scales. The preasymptotic region in the gluon Green’s function extends to about 8 units in rapidity for the transverse scales of the order of 30–100 GeV. To visualize the expected behavior of physical processes with two equal hard scales we calculate the cross section of the process gamma ^{*}+gamma ^{*}rightarrow X to be probed at future very high-energy electron-positron colliders. We find that at gamma ^*gamma ^* energies below 100 ; mathrm{{GeV}} the BFKL Pomeron leads to smaller value of the cross section than the Born approximation, and only starts to dominate at energies about 100 ; mathrm{{GeV}}. This pattern is significantly different from the one which we find using LLx approximation. We also analyze the transverse momentum contributions to the cross section for different virtualities of the photons and find that the dominant contributions to the integral over the transverse momenta comes from lower values than the the external scales in the process under consideration.

Highlights

  • Introduction and motivationOne of the outstanding and interesting problems in the domain of strong interactions is the behavior of the cross sections of hard processes in QCD in the high energy limit

  • We find that the cross section which includes BFKL is lower than the Born cross section for large region of energy which increases with the increase of the scales of the virtual photons

  • The contribution of preasymptotic terms for one hard scale processes is relevant for the diminishing of effective intercept in a wide kinematical range and for the suppressing of onset of BFKL Pomeron at moderate x, or equivalently at moderate energies

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Summary

Introduction and motivation

One of the outstanding and interesting problems in the domain of strong interactions is the behavior of the cross sections of hard processes in QCD in the high energy limit. The strong coupling is fixed in LLx BFKL and practically only starts to run at NLLx level [21] This leads to the large correction, and the increased importance of the infrared regime. We find that even though the impact factors are peaked at the scales of virtualities of the photons, there is significant spread in the transverse momenta along the exchanged Pomeron This leads to the feature that the energy dependence of the resulting cross section is only weakly dependent on the virtualities of the photons. 5 we apply the resummed CCSS solution to the selected process of γ ∗γ ∗ scattering, and analyze the dependence on the energy, polarization, scales and investigate the dominant transverse momenta which contribute to the BFKL Pomeron in this process.

LLx and NLLx BFKL evolution
General setup
Momentum representation
Numerical results for the gluon Green’s function
Findings
Summary and conclusions
Full Text
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