Abstract

The search for the top squark (t˜1) within the kinematic reach of Tevatron Run II is of great contemporary interest. Such a t˜1 can explain the baryon asymmetry of the universe provided 120 GeV⩽mt˜1⩽mt. Moreover if Δm≡mt˜1−mχ˜10 is small, where χ˜10 is the lightest supersymmetric particle (LSP), the dark matter relic density as obtained from the WMAP data may be explained via t˜1-LSP coannihilation. In this scenario the decay t˜1→cχ˜10 is likely to occur with 100% branching ratio but for small Δm the conventional di-jet+E̸T signal becomes unobservable. We propose a new search strategy based on the di-jet+E̸T signature accompanied by an isolated cluster of energy which arises from a decaying heavy particle with characteristic decay length. Our preliminary simulations with Pythia indicate that for 100 GeV⩽mt˜1⩽130 GeV this signal may be observable while somewhat lager mt˜1 may still provide hints of new physics.

Highlights

  • In the Minimal Supersymmetric Standard Model (MSSM) [1] there are two scalar superpartners tL and tR, of the top quark which are the weak eigenstates

  • Due to mixing effects in the top squark mass matrix in the weak basis driven by the top quark mass there may be a significant mass difference between t1 and t2

  • The former could very well be the next-to-lightest supersymmetric particle (NLSP), the lightest neutralino (χ01) being the lightest supersymmetric particle (LSP) by the standard assumption in R-parity conserving MSSM. This happens in a wide region of the MSSM parameter space

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Summary

Introduction

In the Minimal Supersymmetric Standard Model (MSSM) [1] there are two scalar superpartners tL and tR, of the top quark which are the weak eigenstates. As a result the efficiency of the kinematical cuts for suppressing the background as well as that of c-jet tagging decreases. Even in more restricted versions of the MSSM like the minimal supergravity model(mSUGRA) [14] one finds a narrow region of the parameter space where t1 - LSP coannihilation is an important relic density producing mechanism[15].

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