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Cross-section asymmetries around the Z peak

A simple model-independent formula for cross-section asymmetries A in fermion-pair production is derived, which may be used for the analysis of LEP~1 data, A = \sum_n A_n (s - M_Z^2)^n. The coefficient A_0 depends on the Z boson exchange, A_1 additionally on the \gamma Z interference, while the high...

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Autor principal: Riemann, T.
Lenguaje:eng
Publicado: 1992
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(92)90911-M
http://cds.cern.ch/record/239469
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author Riemann, T.
author_facet Riemann, T.
author_sort Riemann, T.
collection CERN
description A simple model-independent formula for cross-section asymmetries A in fermion-pair production is derived, which may be used for the analysis of LEP~1 data, A = \sum_n A_n (s - M_Z^2)^n. The coefficient A_0 depends on the Z boson exchange, A_1 additionally on the \gamma Z interference, while the higher-order contributions are practically redundant. QED corrections are taken into account, and relations to other approaches are indicated.
id cern-239469
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1992
record_format invenio
spelling cern-2394692023-03-14T17:13:01Zdoi:10.1016/0370-2693(92)90911-Mhttp://cds.cern.ch/record/239469engRiemann, T.Cross-section asymmetries around the Z peakParticle Physics - PhenomenologyA simple model-independent formula for cross-section asymmetries A in fermion-pair production is derived, which may be used for the analysis of LEP~1 data, A = \sum_n A_n (s - M_Z^2)^n. The coefficient A_0 depends on the Z boson exchange, A_1 additionally on the \gamma Z interference, while the higher-order contributions are practically redundant. QED corrections are taken into account, and relations to other approaches are indicated.A simple model-independent formula for cross-section asymmetries $A$ in fermion-pair production is derived, which may be used for the analysis of LEP1 data, $A = \sum_n A_n (s - M_Z~2)~n$. The coefficient $A_0$ depends on the $Z$ boson exchange, $A_1$ additionally on the $\gamma Z$ interference, while the higher-order contributions are practically redundant. QED corrections are taken into account, and relations to other approaches are indicated.A simple model-independent formula for cross-section asymmetries $A$ in fermion-pair production is derived, which may be used for the analysis of LEP1 data, $A = \sum_n A_n (s - M_Z~2)~n$. The coefficient $A_0$ depends on the $Z$ boson exchange, $A_1$ additionally on the $\gamma Z$ interference, while the higher-order contributions are practically redundant. QED corrections are taken into account, and relations to other approaches are indicated.A simple model-independent formula for cross-section asymmetries A in fermion-pair production is derived, which may be used for the analysis of LEP 1 data, A = Σ n A n ( s − M Z 2 ) n . The coefficient A 0 depends on the Z boson exchange, A 1 additionally on the γZ interference, while the higher-order contributions are practically redundant. QED corrections are taken into account, and relations to other approaches are indicated.hep-ph/9506382CERN-TH-6590-92CERN-TH-6590-92oai:cds.cern.ch:2394691992
spellingShingle Particle Physics - Phenomenology
Riemann, T.
Cross-section asymmetries around the Z peak
title Cross-section asymmetries around the Z peak
title_full Cross-section asymmetries around the Z peak
title_fullStr Cross-section asymmetries around the Z peak
title_full_unstemmed Cross-section asymmetries around the Z peak
title_short Cross-section asymmetries around the Z peak
title_sort cross-section asymmetries around the z peak
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(92)90911-M
http://cds.cern.ch/record/239469
work_keys_str_mv AT riemannt crosssectionasymmetriesaroundthezpeak