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Large- $N_{c}$ meson theory

We derive an effective Lagrangian for meson fields. This is done in the light-cone gauge for two-dimensional large-N_c QCD by using the bilocal auxiliary field method. The auxiliary fields are bilocal on light-cone space and their Fourier transformation determines the parton momentum distribution. A...

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Detalles Bibliográficos
Autores principales: Kuroki, Shin-Ichiro, Morikawa, Keiichi, Morozumi, Takuya
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:http://cds.cern.ch/record/491582
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author Kuroki, Shin-Ichiro
Morikawa, Keiichi
Morozumi, Takuya
author_facet Kuroki, Shin-Ichiro
Morikawa, Keiichi
Morozumi, Takuya
author_sort Kuroki, Shin-Ichiro
collection CERN
description We derive an effective Lagrangian for meson fields. This is done in the light-cone gauge for two-dimensional large-N_c QCD by using the bilocal auxiliary field method. The auxiliary fields are bilocal on light-cone space and their Fourier transformation determines the parton momentum distribution. As the first test of our method, the 't Hooft equation is derived from the effective Lagrangian.
id cern-491582
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
record_format invenio
spelling cern-4915822023-03-14T20:03:58Zhttp://cds.cern.ch/record/491582engKuroki, Shin-IchiroMorikawa, KeiichiMorozumi, TakuyaLarge- $N_{c}$ meson theoryParticle Physics - TheoryWe derive an effective Lagrangian for meson fields. This is done in the light-cone gauge for two-dimensional large-N_c QCD by using the bilocal auxiliary field method. The auxiliary fields are bilocal on light-cone space and their Fourier transformation determines the parton momentum distribution. As the first test of our method, the 't Hooft equation is derived from the effective Lagrangian.We derive an effective Lagrangian for meson fields. This is done in the light-cone gauge for two-dimensional large-N_c QCD by using the bilocal auxiliary field method. The auxiliary fields are bilocal on light-cone space and their Fourier transformation determines the parton momentum distribution. As the first test of our method, the 't Hooft equation is derived from the effective Lagrangian.hep-th/0103121CERN-TH-2001-070HUPD-0102CERN-TH-2001-070HUPD-2001-02oai:cds.cern.ch:4915822001-03-15
spellingShingle Particle Physics - Theory
Kuroki, Shin-Ichiro
Morikawa, Keiichi
Morozumi, Takuya
Large- $N_{c}$ meson theory
title Large- $N_{c}$ meson theory
title_full Large- $N_{c}$ meson theory
title_fullStr Large- $N_{c}$ meson theory
title_full_unstemmed Large- $N_{c}$ meson theory
title_short Large- $N_{c}$ meson theory
title_sort large- $n_{c}$ meson theory
topic Particle Physics - Theory
url http://cds.cern.ch/record/491582
work_keys_str_mv AT kurokishinichiro largencmesontheory
AT morikawakeiichi largencmesontheory
AT morozumitakuya largencmesontheory