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The BFKL Pomeron within Physical Renormalization Schemes and Scales

In this lecture the next-to-leading order (NLO) corrections to the QCD Pomeron intercept obtained from the Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation are discussed. It is shown that the BFKL Pomeron intercept when evaluated in non-Abelian physical renormalization schemes with Brodsky-Lepage-Macke...

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Detalles Bibliográficos
Autores principales: Fadin, V S, Kim, V T, Lipatov, L N, Pivovarov, G B
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:http://cds.cern.ch/record/573007
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author Fadin, V S
Kim, V T
Lipatov, L N
Pivovarov, G B
author_facet Fadin, V S
Kim, V T
Lipatov, L N
Pivovarov, G B
author_sort Fadin, V S
collection CERN
description In this lecture the next-to-leading order (NLO) corrections to the QCD Pomeron intercept obtained from the Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation are discussed. It is shown that the BFKL Pomeron intercept when evaluated in non-Abelian physical renormalization schemes with Brodsky-Lepage-Mackenzie (BLM) optimal scale setting does not exhibit the serious problems encountered in the modified minimal subtraction (bar{MS}) scheme. The results obtained provide an opportunity for applications of the NLO BFKL resummation to high-energy phenomenology. One of such applications for virtual gamma-gamma total cross section shows a good agreement with preliminary data at CERN LEP.
id cern-573007
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5730072019-09-30T06:29:59Zhttp://cds.cern.ch/record/573007engFadin, V SKim, V TLipatov, L NPivovarov, G BThe BFKL Pomeron within Physical Renormalization Schemes and ScalesParticle Physics - PhenomenologyIn this lecture the next-to-leading order (NLO) corrections to the QCD Pomeron intercept obtained from the Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation are discussed. It is shown that the BFKL Pomeron intercept when evaluated in non-Abelian physical renormalization schemes with Brodsky-Lepage-Mackenzie (BLM) optimal scale setting does not exhibit the serious problems encountered in the modified minimal subtraction (bar{MS}) scheme. The results obtained provide an opportunity for applications of the NLO BFKL resummation to high-energy phenomenology. One of such applications for virtual gamma-gamma total cross section shows a good agreement with preliminary data at CERN LEP.hep-ph/0207296oai:cds.cern.ch:5730072002-07-24
spellingShingle Particle Physics - Phenomenology
Fadin, V S
Kim, V T
Lipatov, L N
Pivovarov, G B
The BFKL Pomeron within Physical Renormalization Schemes and Scales
title The BFKL Pomeron within Physical Renormalization Schemes and Scales
title_full The BFKL Pomeron within Physical Renormalization Schemes and Scales
title_fullStr The BFKL Pomeron within Physical Renormalization Schemes and Scales
title_full_unstemmed The BFKL Pomeron within Physical Renormalization Schemes and Scales
title_short The BFKL Pomeron within Physical Renormalization Schemes and Scales
title_sort bfkl pomeron within physical renormalization schemes and scales
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/573007
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