Non linear evolution: Revisiting the solution in the saturation region

Carlos Contreras; Eugene Levin; Rodrigo Meneses

doi:10.1007/JHEP10(2014)138

Non linear evolution: Revisiting the solution in the saturation region

Carlos Contreras, Eugene Levin^*, Rodrigo Meneses

^*Corresponding author for this work

School of Physics and Astronomy

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Abstract

Abstract: In this paper we revisit the problem of the solution to Balitsky-Kovchegov equation deeply in the saturation domain. We find that solution has the form given in ref. [23] but it depends on variable (equestrian present) Const and the value of Const is calculated in this paper. We propose the solution for full BFKL kernel at large in the entire kinematic region that satisfies the McLerran-Venugopalan-type [3–7] initial condition.

Original language	English
Article number	138
Journal	Journal of High Energy Physics
Volume	2014
Issue number	10
DOIs	https://doi.org/10.1007/JHEP10(2014)138
State	Published - Oct 2014

Keywords

QCD
Resummation

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10.1007/JHEP10(2014)138

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abstract = "Abstract: In this paper we revisit the problem of the solution to Balitsky-Kovchegov equation deeply in the saturation domain. We find that solution has the form given in ref. [23] but it depends on variable (equestrian present) Const and the value of Const is calculated in this paper. We propose the solution for full BFKL kernel at large in the entire kinematic region that satisfies the McLerran-Venugopalan-type [3–7] initial condition.",

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N2 - Abstract: In this paper we revisit the problem of the solution to Balitsky-Kovchegov equation deeply in the saturation domain. We find that solution has the form given in ref. [23] but it depends on variable (equestrian present) Const and the value of Const is calculated in this paper. We propose the solution for full BFKL kernel at large in the entire kinematic region that satisfies the McLerran-Venugopalan-type [3–7] initial condition.

AB - Abstract: In this paper we revisit the problem of the solution to Balitsky-Kovchegov equation deeply in the saturation domain. We find that solution has the form given in ref. [23] but it depends on variable (equestrian present) Const and the value of Const is calculated in this paper. We propose the solution for full BFKL kernel at large in the entire kinematic region that satisfies the McLerran-Venugopalan-type [3–7] initial condition.

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KW - Resummation

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Non linear evolution: Revisiting the solution in the saturation region

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