An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly

A global fit to the recent B → K* μ + μ - data shows indications for a large new-physics contribution to the Wilson coefficient of the semi-leptonic vector operator. In this article we consider a simple Z′-boson model of 3-3-1 type that can accommodate such an effect without violating any other cons...

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Main Authors: Gauld, R, Goertz, F, Haisch, U
Format: Journal article
Published: Springer Berlin Heidelberg 2014
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author Gauld, R
Goertz, F
Haisch, U
author_facet Gauld, R
Goertz, F
Haisch, U
author_sort Gauld, R
collection OXFORD
description A global fit to the recent B → K* μ + μ - data shows indications for a large new-physics contribution to the Wilson coefficient of the semi-leptonic vector operator. In this article we consider a simple Z′-boson model of 3-3-1 type that can accommodate such an effect without violating any other constraint from quark-flavour physics. Implications for yet unobserved decay modes such as B → X s ν v and longstanding puzzles like B → πK are also discussed. The Z′-boson masses required to address the observed anomaly lie in the range of 7 TeV. Such heavy Z′ bosons evade the existing bounds from precision data and direct searches, and will remain difficult to discover even at a high-luminosity LHC. The potential of an ILC as well as the next generation of low-energy parity-violation experiments in constraining the Z′-boson parameter space is also examined. © 2014 The Author(s).
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spelling oxford-uuid:b9f0c45b-7122-4578-9f90-e91f6eac6ee22022-03-27T05:06:29ZAn explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomalyJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:b9f0c45b-7122-4578-9f90-e91f6eac6ee2Symplectic Elements at OxfordSpringer Berlin Heidelberg2014Gauld, RGoertz, FHaisch, UA global fit to the recent B → K* μ + μ - data shows indications for a large new-physics contribution to the Wilson coefficient of the semi-leptonic vector operator. In this article we consider a simple Z′-boson model of 3-3-1 type that can accommodate such an effect without violating any other constraint from quark-flavour physics. Implications for yet unobserved decay modes such as B → X s ν v and longstanding puzzles like B → πK are also discussed. The Z′-boson masses required to address the observed anomaly lie in the range of 7 TeV. Such heavy Z′ bosons evade the existing bounds from precision data and direct searches, and will remain difficult to discover even at a high-luminosity LHC. The potential of an ILC as well as the next generation of low-energy parity-violation experiments in constraining the Z′-boson parameter space is also examined. © 2014 The Author(s).
spellingShingle Gauld, R
Goertz, F
Haisch, U
An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title_full An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title_fullStr An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title_full_unstemmed An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title_short An explicit Z (')-boson explanation of the B -> K (au) mu (+) mu (-) anomaly
title_sort explicit z boson explanation of the b gt k au mu mu anomaly
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