Abstract

Abstract The determination of scalar lepton and gaugino masses is an important part of the programme of spectroscopic studies of Supersymmetry at a high energy e + e − linear collider. In this article we present results of a study of the processes: e + e − → $ \widetilde{e}_R^{+}\widetilde{e}_R^{-} $ → e + e − $ \widetilde{\chi}_1^0\widetilde{\chi}_1^0 $ , e + e − → $ \widetilde{\mu}_R^{+}\widetilde{\mu}_R^{-} $ → μ + μ − $ \widetilde{\chi}_1^0\widetilde{\chi}_1^0 $ , e + e − → $ \widetilde{e}_L^{+}\widetilde{e}_L^{-} $ → e + e − $ \widetilde{\chi}_2^0\widetilde{\chi}_2^0 $ and e + e − → $ {{\widetilde{\nu}}_{\mathrm{e}}}{{\widetilde{\nu}}_{\mathrm{e}}} $ → e + e − $ \widetilde{\chi}_1^{+}\widetilde{\chi}_1^{-} $ in two Supersymmetric benchmark scenarios at $ \sqrt{s} $ =3 TeV and 1.4 TeV at CLIC. We characterize the detector performance, lepton energy resolution and boson mass resolution. We report the accuracy of the production cross section measurements and the $ {{\widetilde{e}}_{\mathrm{R}}} $ , $ {{\widetilde{\mu}}_{\mathrm{R}}} $ , $ {{\widetilde{\nu}}_{\mathrm{e}}} $ , $ \widetilde{\chi}_1^{\pm } $ , and $ \widetilde{\chi}_1^0 $ mass determinations, estimate the systematic errors affecting the mass measurement and discuss the requirements on the detector time stamping capability and beam polarization. The analysis accounts for the CLIC beam energy spectrum and the dominant beam-induced background. The detector performances are incorporated by full simulation and reconstruction of the events within the framework of the CLIC ILD CDR detector concept.

Highlights

  • 500 1000 1500 2000 2500 3000 3500 4000 Energy: E ( μ+,μ- ) [GeV]200 400 600 800 1000 1200 1400 1600 1800 Vector sum: PT ( μ+,μ- ) [GeV](1/N) dN / 54.8 GeV (1/N)Algebraic sum P (μ+,μ-) [GeV] ) TInvariant mass: M ( μ+,μ- ) [GeV](1/N) dN / 3.01 deg20 40 60 80 100 120 140 160 180 Acolinearity: θ( μ+,μ- ) [deg] fPolar angle of vector sum of the leptons cosθ(μ+,μ-) ) Figure e+e− →9μ.+RDμ−Riscartim√insa=tin3gTveaVr:iadbilmesuounseednteorgsyep(aa)r,atdeimsiugonnalpaTnvdecbtaocrkgsuromun(bd)e, vdeinmtusofnorptThealpgerobcreasics sum (c), dimuon invariant mass (d), acollinearity (e) and polar angle of the vector sum of the leptons (f)

  • The accuracy of the slepton and gaugino mass determination and of the process cross section measurement in pair produced eR, eL, μR, and νe processes has been studied at aCtL√ICs with the = 3 TeV

  • The electron and muon energy resolution and the boson mass resolution are not affected by the beam induced background, provided the detectors have timing capabilities of the order of 1 nsec allowing for the application of particle flow objets (PFO) selection cuts

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Summary

TeV at CLIC

Thomsond and E. van der Kraaija aCERN, CH-1211 Geneva, Switzerland bSanta Cruz Institute of Particle Physics, University of California, Santa Cruz, CA 95064, USA cLaboratoire d’Annecy-le-Vieux de Physique des Particules, Annecy-le-Vieux, France dCavendish Laboratory, University of Cambridge, Cambridge, U.K

Event simulation
Event reconstruction
Two lepton final states
Two leptons and four jets final states
Reconstruction with beam-induced Background
Event selection
Background
Systematic uncertainty related to the event selection
Systematic uncertainty related to the luminosity spectrum
Polarization
Findings
Summary
Full Text
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