The missing gauge conditions for the dual fermion emission vertex and their consequences

The authors find that the dual vertex for emitting a ground state fermion of mass m converts between generalized mesonic G gauges and generalized fermionic F gauges. These generalized gauges consist of infinite linear combinations of F's and G's which are, roughly speaking, square roots of...

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Detalles Bibliográficos
Autores principales: Brink, L, Olive, D, Rebbi, C, Scherk, J
Lenguaje:eng
Publicado: 1973
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(73)90060-9
http://cds.cern.ch/record/880646
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author Brink, L
Olive, D
Rebbi, C
Scherk, J
author_facet Brink, L
Olive, D
Rebbi, C
Scherk, J
author_sort Brink, L
collection CERN
description The authors find that the dual vertex for emitting a ground state fermion of mass m converts between generalized mesonic G gauges and generalized fermionic F gauges. These generalized gauges consist of infinite linear combinations of F's and G's which are, roughly speaking, square roots of Virasoro gauges and exhibit partial reflection and transmission behaviour at the vertex. One of these Ward identities allows us to re-express the amplitude for fermion re- emission in the F/sub 2/ representation where the limit m=0 is well defined. If m=0 and d=10 certain meson channels are saturated by physical (ghost free) states. (12 refs).
id cern-880646
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1973
record_format invenio
spelling cern-8806462019-09-30T06:29:59Zdoi:10.1016/0370-2693(73)90060-9http://cds.cern.ch/record/880646engBrink, LOlive, DRebbi, CScherk, JThe missing gauge conditions for the dual fermion emission vertex and their consequencesParticle Physics - PhenomenologyThe authors find that the dual vertex for emitting a ground state fermion of mass m converts between generalized mesonic G gauges and generalized fermionic F gauges. These generalized gauges consist of infinite linear combinations of F's and G's which are, roughly speaking, square roots of Virasoro gauges and exhibit partial reflection and transmission behaviour at the vertex. One of these Ward identities allows us to re-express the amplitude for fermion re- emission in the F/sub 2/ representation where the limit m=0 is well defined. If m=0 and d=10 certain meson channels are saturated by physical (ghost free) states. (12 refs).CERN-TH-1695oai:cds.cern.ch:8806461973
spellingShingle Particle Physics - Phenomenology
Brink, L
Olive, D
Rebbi, C
Scherk, J
The missing gauge conditions for the dual fermion emission vertex and their consequences
title The missing gauge conditions for the dual fermion emission vertex and their consequences
title_full The missing gauge conditions for the dual fermion emission vertex and their consequences
title_fullStr The missing gauge conditions for the dual fermion emission vertex and their consequences
title_full_unstemmed The missing gauge conditions for the dual fermion emission vertex and their consequences
title_short The missing gauge conditions for the dual fermion emission vertex and their consequences
title_sort missing gauge conditions for the dual fermion emission vertex and their consequences
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(73)90060-9
http://cds.cern.ch/record/880646
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AT scherkj themissinggaugeconditionsforthedualfermionemissionvertexandtheirconsequences
AT brinkl missinggaugeconditionsforthedualfermionemissionvertexandtheirconsequences
AT olived missinggaugeconditionsforthedualfermionemissionvertexandtheirconsequences
AT rebbic missinggaugeconditionsforthedualfermionemissionvertexandtheirconsequences
AT scherkj missinggaugeconditionsforthedualfermionemissionvertexandtheirconsequences

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