Abstract

We consider the effects of R-parity violation due to the inclusion of a bilinear $\mu^\prime L H_u$ superpotential term in high scale supersymmetric models with an EeV scale gravitino as dark matter. Although the typical phenomenological limits on this coupling (e.g. due to lepton number violation and the preservation of the baryon asymmetry) are relaxed when the supersymmetric mass spectrum is assumed to be heavy (in excess of the inflationary scale of $3 \times 10^{13}$ GeV), the requirement that the gravitino be sufficiently long-lived so as to account for the observed dark matter density, leads to a relatively strong bound on $\mu^\prime \lesssim 20$ GeV. The dominant decay channels for the longitudinal component of the gravitino are $Z \nu, W^\pm l^\mp$, and $h\nu$. To avoid an excess neutrino signal in IceCube, our limit on $\mu'$ is then strengthened to $\mu' \lesssim 50$ keV. When the bound is saturated, we find that there is a potentially detectable flux of mono-chromatic neutrinos with EeV energies.

Highlights

  • Naturalness and potential solutions to low-energy phenomenological quandaries such as the discrepancy between the theoretical and experimental determinations of the anomalous magnetic moment of the muon [1,2] pointed to low-energy supersymmetry

  • If supersymmetry plays a role in nature below the Planck scale, it may still be broken at some high energy scale [6]

  • While much of the high-energy physics community would be overjoyed with the detection of weak-scale supersymmetry at the LHC, we have no guarantee that the sparticle spectrum lies within the reach of the LHC

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Summary

INTRODUCTION

Naturalness and potential solutions to low-energy phenomenological quandaries such as the discrepancy between the theoretical and experimental determinations of the anomalous magnetic moment of the muon [1,2] pointed to low-energy supersymmetry. We include a single RPV interaction, generated by the LHu bilinear term in the superpotential This term is sufficient to allow for the decay of the LSP gravitino, and demanding that it remains long lived to account for the dark matter, will enable us to set a limit on the “μ” term associated with this bilinear. We will compare this limit with the one imposed from the preservation of the baryon asymmetry in both weak-scale and high-scale supersymmetry models.

SOME PRELIMINARIES
R-PARITY VIOLATION
Induced mixing
CA: ð16Þ sξ sξ
Constraints on other relevant operators
Limits from lepton number violation
GRAVITINO DECAY
Γðψ μ i
Planck constraints
IceCube constraints
Signatures at the ANITA experiment?
CONCLUSIONS
Full Text
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