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Solving the BFKL Equation with Running Coupling

We describe a formalism for solving the BFKL equation with a coupling that runs for momenta above a certain infrared cutoff. By suitably choosing matching conditions proper account is taken of the fact that the BFKL diffusion implies that the solution in the infrared (fixed coupling) regime depends...

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Detalles Bibliográficos
Autores principales: Forshaw, Jeffrey R., Ross, D.A., Sabio Vera, Agustin
Lenguaje:eng
Publicado: 2000
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(00)01386-1
http://cds.cern.ch/record/475568
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author Forshaw, Jeffrey R.
Ross, D.A.
Sabio Vera, Agustin
author_facet Forshaw, Jeffrey R.
Ross, D.A.
Sabio Vera, Agustin
author_sort Forshaw, Jeffrey R.
collection CERN
description We describe a formalism for solving the BFKL equation with a coupling that runs for momenta above a certain infrared cutoff. By suitably choosing matching conditions proper account is taken of the fact that the BFKL diffusion implies that the solution in the infrared (fixed coupling) regime depends upon the solution in the ultraviolet (running coupling) regime and vice versa. Expanding the BFKL kernel to a given order in the ratio of the transverse momenta allows arbitrary accuracy to be achieved.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2000
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spelling cern-4755682023-03-14T20:37:55Zdoi:10.1016/S0370-2693(00)01386-1http://cds.cern.ch/record/475568engForshaw, Jeffrey R.Ross, D.A.Sabio Vera, AgustinSolving the BFKL Equation with Running CouplingParticle Physics - PhenomenologyWe describe a formalism for solving the BFKL equation with a coupling that runs for momenta above a certain infrared cutoff. By suitably choosing matching conditions proper account is taken of the fact that the BFKL diffusion implies that the solution in the infrared (fixed coupling) regime depends upon the solution in the ultraviolet (running coupling) regime and vice versa. Expanding the BFKL kernel to a given order in the ratio of the transverse momenta allows arbitrary accuracy to be achieved.We describe a formalism for solving the BFKL equation with a coupling that runs for momenta above a certain infrared cutoff. By suitably choosing matching conditions proper account is taken of the fact that the BFKL diffusion implies that the solution in the infrared (fixed coupling) regime depends upon the solution in the ultraviolet (running coupling) regime and vice versa. Expanding the BFKL kernel to a given order in the ratio of the transverse momenta allows arbitrary accuracy to be achieved.hep-ph/0011047MC-TH-00-11CAVENDISH-HEP-2000-11CERN-TH-2000-354CAVENDISH-HEP-2000-11CERN-TH-2000-354MC-TH-2000-11oai:cds.cern.ch:4755682000-11-03
spellingShingle Particle Physics - Phenomenology
Forshaw, Jeffrey R.
Ross, D.A.
Sabio Vera, Agustin
Solving the BFKL Equation with Running Coupling
title Solving the BFKL Equation with Running Coupling
title_full Solving the BFKL Equation with Running Coupling
title_fullStr Solving the BFKL Equation with Running Coupling
title_full_unstemmed Solving the BFKL Equation with Running Coupling
title_short Solving the BFKL Equation with Running Coupling
title_sort solving the bfkl equation with running coupling
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(00)01386-1
http://cds.cern.ch/record/475568
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