Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$

For pt.I see ibid., vol.B185, p.61 (1981). In technicolour models, a charged pseudo-Goldstone boson P/sup +/ receives no mass from order alpha electroweak effects in order alpha /sup 2/, however, a finite mass is generated. The authors compute this order alpha /sup 2/ electroweak contribution, using...

Descripción completa

Detalles Bibliográficos
Autores principales: Chadha, S, Peskin, Michael E
Lenguaje:eng
Publicado: 1981
Materias:
Particle Physics - Theory
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(81)90475-2
http://cds.cern.ch/record/134362
_version_ 1780879757456441344
author Chadha, S
Peskin, Michael E
author_facet Chadha, S
Peskin, Michael E
author_sort Chadha, S
collection CERN
description For pt.I see ibid., vol.B185, p.61 (1981). In technicolour models, a charged pseudo-Goldstone boson P/sup +/ receives no mass from order alpha electroweak effects in order alpha /sup 2/, however, a finite mass is generated. The authors compute this order alpha /sup 2/ electroweak contribution, using chiral perturbation theory in models with SU(N)*SU(N) and SU(2N) chiral symmetry. In the latter case, part of the P/sup +/ mass arises from the nonlinear interactions of pseudo- Goldstone bosons with one another. (12 refs).
id cern-134362
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1981
record_format invenio
spelling cern-1343622019-09-30T06:29:59Zdoi:10.1016/0550-3213(81)90475-2http://cds.cern.ch/record/134362engChadha, SPeskin, Michael EImplications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$Particle Physics - TheoryFor pt.I see ibid., vol.B185, p.61 (1981). In technicolour models, a charged pseudo-Goldstone boson P/sup +/ receives no mass from order alpha electroweak effects in order alpha /sup 2/, however, a finite mass is generated. The authors compute this order alpha /sup 2/ electroweak contribution, using chiral perturbation theory in models with SU(N)*SU(N) and SU(2N) chiral symmetry. In the latter case, part of the P/sup +/ mass arises from the nonlinear interactions of pseudo- Goldstone bosons with one another. (12 refs).CERN-TH-3038oai:cds.cern.ch:1343621981-02-26
spellingShingle Particle Physics - Theory
Chadha, S
Peskin, Michael E
Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title_full Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title_fullStr Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title_full_unstemmed Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title_short Implications of chiral dynamics in theories of technicolour ; 2, the mass of the P$^{+}$
title_sort implications of chiral dynamics in theories of technicolour ; 2, the mass of the p$^{+}$
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(81)90475-2
http://cds.cern.ch/record/134362
work_keys_str_mv AT chadhas implicationsofchiraldynamicsintheoriesoftechnicolour2themassofthep
AT peskinmichaele implicationsofchiraldynamicsintheoriesoftechnicolour2themassofthep

Ejemplares similares