Abstract

Supersymmetry (SUSY) with bilinearly broken \(R\) parity (bRPV) offers an attractive possibility to explain the origin of neutrino masses and mixings. In such scenarios, the study of neutralino decays at colliders gives access to neutrino sector parameters. The ILC offers a very clean environment to study the neutralino properties as well as its subsequent decays, which typically involve a \(W\) or \(Z\) boson and a lepton. This study is based on ILC beam parameters according to the Technical Design Report for a center of mass energy of \(500~\hbox {GeV}\). A full detector simulation of the International Large Detector (ILD) has been performed for all Standard Model backgrounds and for neutralino pair production within a simplified model. The bRPV parameters are fixed according to current neutrino data. In this scenario, the \(\tilde{\chi }^0_1\) mass can be reconstructed with an uncertainty of \(\delta m^{{\mathrm {fit}}}_{\widetilde{\chi }^{0}_{1}}=(40\text {(stat.)} \oplus 50\text {(syst.)})~\hbox {MeV}\) for an integrated luminosity of \(500\,\hbox {fb}^{-1}\) from direct \(\tilde{\chi }^0_1\) pair production, thus, to a large extent independently of the rest of the SUSY spectrum. The achievable precision on the atmospheric neutrino mixing angle \(\sin ^2 \theta _{23}\) from measuring the neutralino branching fractions BR(\(\tilde{\chi }_1^0\rightarrow W\mu \)) and BR(\(\tilde{\chi }_1^0\rightarrow W \tau \)) at the ILC is in the same range than current uncertainties from neutrino experiments. Thus, the ILC could have the opportunity to unveil the mechanism of neutrino mass generation.

Highlights

  • The presence of all these terms would lead to proton decay, which is experimentally not observed

  • The muons originating from an lightest SUSY particle (LSP) decay carry a momentum of up to 80 GeV, while the jets originating from the W bosons from the signal decay have an energy of up to 200 GeV

  • The μμ channel shows a clear signal peak, which can be used for measuring the LSP mass accurately

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Summary

Introduction

The presence of all these terms would lead to proton decay, which is experimentally not observed. A common way to circumvent this problem is to introduce a discrete Z2 symmetry assigned to each field in order to suppress these terms. This quantum number, called R parity, has the form R = (−1)3B+L+2S, (1). SM particles always carry R = +1 and SUSY particles R = −1 The conservation of this quantum number has the consequence that all B and L breaking terms in the SUSY Lagrangian are forbidden and the proton remains stable. The muons originating from an LSP decay carry a momentum of up to 80 GeV, while the jets originating from the W bosons from the signal decay have an energy of up to 200 GeV.

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