Abstract

String theory has no parameter except the string scale MS, so the Planck scale MPl, the supersymmetry-breaking scale , the electroweak scale mEW as well as the vacuum energy density (cosmological constant) Λ are to be determined dynamically at any local minimum solution in the string theory landscape. Here we consider a model that links the supersymmetric electroweak phenomenology (bottom up) to the string theory motivated flux compactification approach (top down). In this model, supersymmetry is broken by a combination of the racetrack Kähler uplift mechanism, which naturally allows an exponentially small positive Λ in a local minimum, and the anti-D3-brane in the KKLT scenario. In the absence of the Higgs doublets from the supersymmetric standard model, one has either a small Λ or a big enough , but not both. The introduction of the Higgs fields (with their soft terms) allows a small Λ and a big enough simultaneously. Since an exponentially small Λ is statistically preferred (as the properly normalized probability distribution P(Λ) diverges at Λ = 0+), identifying the observed Λobs to the median value Λ50% yields mEW∼ 100 GeV. We also find that the warped anti-D3-brane tension has a SUSY-breaking scale ∼ 100 mEW while the SUSY-breaking scale that directly correlates with the Higgs fields in the visible sector is ≃ mEW.

Highlights

  • Which displays some of the most relevant operators that are known to be present in nature

  • String theory has no parameter except the string scale MS, so the Planck scale MPl, the supersymmetry-breaking scale m$su$sy, the electroweak scale mEW as well as the vacuum energy density Λ are to be determined dynamically at any local minimum solution in the string theory landscape

  • We find that the warped anti-D3-brane tension has a SUSY-breaking scale M$su$sy ∼ 100 mEW while the SUSY-breaking scale that directly correlates with the Higgs fields in the visible sector is m$su$sy mEW

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Summary

The model

Let us present the effective potential in our simplified model. The relation between the string scale MS and MPl is given in terms of the dimensionless compactified volume V, which is related to the Kähler modulus T given by. The warped D3-brane tension explicitly breaks SUSY and gives a SUSYbreaking scale, T3 ∼ M$s4u$sy, which are assumed to generate the various soft terms in Sh in the Higgs potential. This negative Higgs contribution cancels the positive uplift from the D3-brane tension and allows a positive exponentially small cosmological constant We present these three terms here: pT3 + T)n. (2) If the Higgs field terms Sh and Dh are not included, the upper bound on Dreduces to an upper bound on the D3-brane tension, and the SUSY-breaking scale will be negligibly small. (3) If an D3-brane is not included, the SUSY-breaking scale from the ξ-term would be exponentially small; and the Higgs potential will push the ground state to an AdS vacuum with |Λ| Λobs. We are mostly interested in the branch with dS solutions

Analysis
Statistical preference for a small positive Λ
Positive D
Negative D
Supersymmetric standard model
Relation between EW scale and SUSY-breaking scale
Comments
Discussion and remarks
Summary and conclusion
A T -Dependence of the D3-brane term and the Higgs terms
B Single uplift model
C Racetrack model with single uplift
D Racetrack model with combined uplift
Findings
E Explicit calculation and approximation
H Statistical analysis
Full Text
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