Abstract

In the context of supersymmetric models where the gauginos may have both Majorana and Dirac masses we investigate the general constraints from flavour-changing processes on the scalar mass matrices. One finds that the chirality-flip suppression of flavour-changing effects usually invoked in the pure Dirac case holds in the mass insertion approximation but not in the general case, and fails in particular for inverted hierarchy models. We quantify the constraints in several flavour models which correlate fermion and scalar superpartner masses. We also discuss the limit of very large Majorana gaugino masses compared to the chiral adjoint and Dirac masses, where the remaining light eigenstate is the “fake” gaugino, including the consequences of suppressed couplings to quarks beyond flavour constraints.

Highlights

  • Supersymmetric extensions of the Standard Model are arguably still the most plausible ways to deal with the various mysteries of the Standard Model

  • Dudas et al / Nuclear Physics B 884 (2014) 632–671 at LHC for the time being suggests, that we should seriouslyconsider non-minimal extensions compared to the minimal supersymmetric extension (MSSM) in all its various forms

  • In models in which the scale of mediation of supersymmetry breaking is similar or higher than the scale of flavour symmetry breaking, fermion masses and mixing hierarchies are correlated with the flavour structure of superpartners

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Summary

Introduction

The simplest models based on a single abelian flavoured gauge group, providing an approximate alignment mechanism for scalar mass matrices, still require scalar partners heavier than at least 100 TeV Both collider and flavour constraints encourage us to search for non-minimal extensions with suppressed collider bounds and flavour-changing transitions. This happens when the Majorana gaugino mass is much bigger than the Dirac and the adjoint fermion masses.

Neutral meson mixing in supersymmetry with Dirac gauginos
Effective Hamiltonian
Flavour-violation observables
Flavour patterns
Degeneracy – mass insertion approximation
Alignment
Bounds in the mass insertion approximation
Majorana gluino
Dirac gluino
Fake gluino
Beyond the mass insertion approximation
Dirac versus Majorana
Alignment in both left and right sectors
Inverted hierarchy
Including the first two generations
10 TeV 2 f5
A diversion: how to fake a gluino
B Σ m 2Σ
Phenomenological consequences
Conclusions
From the Lagrangian to Feynman rules
Abelian models
Non-abelian extension
Mass insertion approximation
Decoupled first two generations
B2 B3 B4 B5

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