Abstract

Large numbers of muons will be produced at facilities developed to probe lepton flavor violating process $\mu\to e\gamma$. We show that by constructing a suitable asymmetry, radiative muon decay $\mu\to e \gamma\nu_\mu\bar{\nu}_e$ can also be used to test the $WW\gamma$ vertex at such facilities. The process has two missing neutrinos in the final state and on integrating their momenta, the partial differential decay rate shows no radiation-amplitude-zero. We establish, however, that an easily separable part of the normalized differential decay rate, odd under the exchange of photon and electron energies, does have a zero in the case of standard model (SM). This "new type of zero" has hitherto not been studied in literature. A suitably constructed asymmetry using this fact, enables a sensitive probe for the $WW\gamma$ vertex beyond the SM. With a simplistic analysis, we find that the $C$ and $P$ conserving dimension four $WW\gamma$ vertex can be probed at ${\cal O}(10^{-2})$ with satisfactory significance level.

Highlights

  • INTRODUCTIONThe SUð2ÞL ⊗ Uð1ÞY theory of electroweak interactions has been tested extensively in last few decades and there is no doubt that it is the correct theory at least up to the TeV scale

  • The SUð2ÞL ⊗ Uð1ÞY theory of electroweak interactions has been tested extensively in last few decades and there is no doubt that it is the correct theory at least up to the TeV scale. This conviction is largely based on the precision measurements at LEP and the consistency of the top and Higgs boson masses which could be predicted by taking radiative corrections into account

  • We have shown that radiative muon decay μ → eγνμνe is a promising mode to probe loop-level corrections in the standard model (SM) to the C- and P-conserving dimensionfour WWγ vertex with good accuracy

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Summary

INTRODUCTION

The SUð2ÞL ⊗ Uð1ÞY theory of electroweak interactions has been tested extensively in last few decades and there is no doubt that it is the correct theory at least up to the TeV scale This conviction is largely based on the precision measurements at LEP and the consistency of the top and Higgs boson masses which could be predicted by taking radiative corrections into account. Radiative muon decay μ → eγνμνe is a promising mode to measure the true magnetic moment (due to a real photon in the final state) of the W boson in this regard. II we briefly discuss the decay kinematics and relevant expressions for the decay rate

THEORETICAL FRAMEWORK
OBSERVABLE AND ASYMMETRY
SIMULATION AND ANALYSIS
CONCLUSION
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