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Deflected Mirage Mediation: A Framework for Generalized Supersymmetry Breaking

Lisa L. Everett, Ian-Woo Kim, Peter Ouyang, Kathryn M. Zurek

TL;DR

A general phenomenological framework for dialing between gravity mediation, gauge mediation, and anomaly mediation is presented, which provides a rich setting in which to explore generalized supersymmetry breaking at the CERN Large Hadron Collider.

Abstract

We present a general phenomenological framework for dialing between gravity mediation, gauge mediation, and anomaly mediation. The approach is motivated from recent developments in moduli stabilization, which suggest that gravity mediated terms can be effectively loop suppressed and thus comparable to gauge and anomaly mediated terms. The gauginos exhibit a mirage unification behavior at a "deflected" scale, and gluinos are often the lightest colored sparticles. The approach provides a rich setting in which to explore generalized supersymmetry breaking at the LHC.

Deflected Mirage Mediation: A Framework for Generalized Supersymmetry Breaking

TL;DR

A general phenomenological framework for dialing between gravity mediation, gauge mediation, and anomaly mediation is presented, which provides a rich setting in which to explore generalized supersymmetry breaking at the CERN Large Hadron Collider.

Abstract

We present a general phenomenological framework for dialing between gravity mediation, gauge mediation, and anomaly mediation. The approach is motivated from recent developments in moduli stabilization, which suggest that gravity mediated terms can be effectively loop suppressed and thus comparable to gauge and anomaly mediated terms. The gauginos exhibit a mirage unification behavior at a "deflected" scale, and gluinos are often the lightest colored sparticles. The approach provides a rich setting in which to explore generalized supersymmetry breaking at the LHC.

Paper Structure

This paper contains 17 equations, 2 figures, 1 table.

Figures (2)

  • Figure 1: The renormalization group evolution of the gaugino masses (top panel) and the soft scalar masses (bottom panel) of the first generation for point A, in which $M_{\rm mess}=10^{12}\hbox{GeV}$. For the scalar masses, $M_{fi}\equiv m^2_{fi}/\sqrt{|m^2_{fi}|}$.
  • Figure 2: The renormalization group evolution of the gaugino masses (top panel) and the first generation soft scalar masses (bottom panel) for Point B, in which $M_{\rm mess}=10^8\hbox{GeV}$.