Abstract

We calculate the rare fluctuations of the $S$-matrix on top of the full next-to-leading order corrections in the center of mass frame. The relevant result in the saturation regime shows that the exponential factor of the $S$-matrix is $\sqrt{2}$ as large as the result which emerges when the rare fluctuation effects are taken into account. We find that the factor of $\sqrt{2}$ change of the exponential factor is induced by the gluon loop corrections which compensate part of rapidity decrease of the $S$-matrix made by quark loops and lead to the rare fluctuations becoming important again. To ensure the relevant results of the $S$-matrix are independent of the frame choice, the rare fluctuations of the $S$-matrix are also derived in a general frame. It is found that all the results are consistent with each other in both frames.

Highlights

  • In high-energy QCD, one of the most challenging problem has been to study theoretically and experimentally the parton saturation

  • In the fixed coupling case, the S matrix obtained from the BK equation shows a quadratic rapidity dependence in its exponent, and it was found that the exponential factor of the S matrix (∼ exp 1⁄2−c1α 2sðY − Y0Þ2=2Š) is twice as large as the one which takes into account the rare fluctuation effects [20], where αs is the coupling constant, and c1 is a constant which is not important in this paper

  • To reveal which one is the dominant effect, we studied the rare fluctuations on top of the running coupling effect in Ref. [11]

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Summary

INTRODUCTION

In high-energy QCD, one of the most challenging problem has been to study theoretically and experimentally the parton saturation. In the fixed coupling case, the S matrix obtained from the BK equation shows a quadratic rapidity dependence in its exponent, and it was found that the exponential factor of the S matrix (∼ exp 1⁄2−c1α 2sðY − Y0Þ2=2Š) is twice as large as the one which takes into account the rare fluctuation effects [20], where αs is the coupling constant, and c1 is a constant which is not important in this paper This result shows that the rare fluctuations reduce the evolution speed of the dipole scattering amplitude with respect to rapidity. The result shows that the influence of the rare fluctuations in the NLO BK case on the S matrix are greater than that in the running coupling BK case, which indicates that the rare fluctuations are important in the NLO BK case, it is not as significant as the LO BK case

LEADING-ORDER EVOLUTION EQUATION
Balitsky-Kovchegov equation
NEXT-TO-LEADING-ORDER EVOLUTION EQUATION
Analytic solution in the saturation region
Leading-order case
EFFECTS OF RARE FLUCTUATIONS IN HIGH-ENERGY DIPOLE-DIPOLE SCATTERING
Next-to-leading-order case
In the case of running coupling
In the case of full next-to-leading order
Z R21 2R20
Full Text
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