Predicting the SUSY breaking scale in SUGRA models with degenerate vacua

Author:

Froggatt C. D.1,Nevzorov R.2ORCID,Nielsen H. B.3,Thomas A. W.4

Affiliation:

1. School of Physics and Astronomy, University of Glasgow, Glasgow G12 8QQ, UK

2. NRC Kurchatov Institute – ITEP, Moscow 117218, Russia

3. The Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, Copenhagen DK-2100, Denmark

4. ARC Centre of Excellence for Particle Physics at the Terascale and CSSM, Department of Physics, The University of Adelaide, Adelaide SA 5005, Australia

Abstract

In [Formula: see text] supergravity, the scalar potential may have supersymmetric (SUSY) and nonsupersymmetric Minkowski vacua (associated with supersymmetric and physical phases) with vanishing energy density. In the supersymmetric Minkowski (second) phase, some breakdown of SUSY may be induced by nonperturbative effects in the observable sector that give rise to a tiny positive vacuum energy density. Postulating the exact degeneracy of the physical and second vacua as well as assuming that at high energies the couplings in both phases are almost identical, one can estimate the dark energy density in these vacua. It is mostly determined by the SUSY breaking scale [Formula: see text] in the physical phase. Exploring the two-loop renormalization group (RG) flow of couplings in these vacua, we find that the measured value of the cosmological constant can be reproduced if [Formula: see text] varies from 20 TeV to 400 TeV. We also argue that this prediction for the SUSY breaking scale is consistent with the upper bound on [Formula: see text] in the higgsino dark matter scenario.

Funder

Australian Research Council

Publisher

World Scientific Pub Co Pte Lt

Subject

Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics

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3. D. L. Bennett, C. D. Froggatt and H. B. Nielsen, Perspectives in Particle Physics ’94, eds. D. Klabuc̆ar, I. Picek and D. Tadić (World Scientific, 1995), p. 255, arXiv:hep-ph/9504294.

4. Standard model criticality prediction top mass 173 ± 5 GeV and Higgs mass 135 ± 9 GeV

5. Implementation of the multiple point principle in the two-Higgs doublet model of type II

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