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Predictions for ${\bar \nu} \nu \gamma$ Production at LEP

We study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop corrections are taken into account and higher order contributions, in particular those for the observed real photons, are added whenever necessary. The event generator \KK MC, a general-purpose Monte...

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Detalles Bibliográficos
Autores principales: Bardin, D., Jadach, S., Riemann, T., Was, Z.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1007/s100520200948
http://cds.cern.ch/record/524717
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author Bardin, D.
Jadach, S.
Riemann, T.
Was, Z.
author_facet Bardin, D.
Jadach, S.
Riemann, T.
Was, Z.
author_sort Bardin, D.
collection CERN
description We study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop corrections are taken into account and higher order contributions, in particular those for the observed real photons, are added whenever necessary. The event generator \KK MC, a general-purpose Monte Carlo generator for the process $e^+e^- \to \bar f f n\gamma$ based on the method of exclusive exponentiation, is used as the environment. We extend its applicability to the process $e^+e^- \to \bar \nu_l \nu_l n\gamma$, $l=e,\mu,\tau$, where the observation of at least a single $\gamma$ is required. The exponentiation is implemented in much the same way as for the s-channel process alone. In particular, all photonic effects present in the case of W exchange, which {\it cannot} be included in the s-channel exponentiation scheme, are calculated to a finite order only. The real hard photon matrix element is calculated up to ${\cal O} ({\alpha^2})$. Leading logarithmic contributions of the two-loop corrections and one-loop photonic corrections accompanying real single photon emission are included. The electroweak corrections are calculated with the DIZET library of the ZFITTER package. Numerical tests and predictions for typical observables are presented.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
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spelling cern-5247172023-03-14T20:20:12Zdoi:10.1007/s100520200948http://cds.cern.ch/record/524717engBardin, D.Jadach, S.Riemann, T.Was, Z.Predictions for ${\bar \nu} \nu \gamma$ Production at LEPParticle Physics - PhenomenologyWe study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop corrections are taken into account and higher order contributions, in particular those for the observed real photons, are added whenever necessary. The event generator \KK MC, a general-purpose Monte Carlo generator for the process $e^+e^- \to \bar f f n\gamma$ based on the method of exclusive exponentiation, is used as the environment. We extend its applicability to the process $e^+e^- \to \bar \nu_l \nu_l n\gamma$, $l=e,\mu,\tau$, where the observation of at least a single $\gamma$ is required. The exponentiation is implemented in much the same way as for the s-channel process alone. In particular, all photonic effects present in the case of W exchange, which {\it cannot} be included in the s-channel exponentiation scheme, are calculated to a finite order only. The real hard photon matrix element is calculated up to ${\cal O} ({\alpha^2})$. Leading logarithmic contributions of the two-loop corrections and one-loop photonic corrections accompanying real single photon emission are included. The electroweak corrections are calculated with the DIZET library of the ZFITTER package. Numerical tests and predictions for typical observables are presented.We study predictions for the reaction $e^+e^- \to {\bar \nu} \nu (n \gamma)$. The complete one-loop corrections are taken into account and higher order contributions, in particular those for the observed real photons, are added whenever necessary. The event generator \KK MC, a general-purpose Monte Carlo generator for the process $e^+e^- \to \bar f f n\gamma$ based on the method of exclusive exponentiation, is used as the environment. We extend its applicability to the process $e^+e^- \to \bar \nu_l \nu_l n\gamma$, $l=e,\mu,\tau$, where the observation of at least a single $\gamma$ is required. The exponentiation is implemented in much the same way as for the s-channel process alone. In particular, all photonic effects present in the case of W exchange, which {\it cannot} be included in the s-channel exponentiation scheme, are calculated to a finite order only. The real hard photon matrix element is calculated up to ${\cal O} ({\alpha^2})$. Leading logarithmic contributions of the two-loop corrections and one-loop photonic corrections accompanying real single photon emission are included. The electroweak corrections are calculated with the DIZET library of the ZFITTER package. Numerical tests and predictions for typical observables are presented.hep-ph/0110371CERN-TH-2001-161DESY-01-005CERN-TH-2001-161DESY-2001-005DESY-01-005oai:cds.cern.ch:5247172001-10-29
spellingShingle Particle Physics - Phenomenology
Bardin, D.
Jadach, S.
Riemann, T.
Was, Z.
Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title_full Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title_fullStr Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title_full_unstemmed Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title_short Predictions for ${\bar \nu} \nu \gamma$ Production at LEP
title_sort predictions for ${\bar \nu} \nu \gamma$ production at lep
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/s100520200948
http://cds.cern.ch/record/524717
work_keys_str_mv AT bardind predictionsforbarnunugammaproductionatlep
AT jadachs predictionsforbarnunugammaproductionatlep
AT riemannt predictionsforbarnunugammaproductionatlep
AT wasz predictionsforbarnunugammaproductionatlep