Abstract

In anomaly-mediated supersymmetry breaking models, superpartner masses are proportional to couplings squared. Their hidden sectors therefore naturally contain WIMPless dark matter, particles whose thermal relic abundance is guaranteed to be of the correct size, even though they are not weakly interacting massive particles. We study viable dark matter candidates in WIMPless anomaly-mediated supersymmetry breaking models with non-Abelian hidden sectors and highlight unusual possibilities that emerge in even the simplest models. In one example with a pure $SU(N)$ hidden sector, stable hidden gluinos freeze out with the correct relic density, but have an extremely low, but natural, confinement scale, providing a framework for self-interacting dark matter. In another simple scenario, hidden gluinos freeze out and decay to visible Winos with the correct relic density, and hidden glueballs may either be stable, providing a natural framework for mixed cold-hot dark matter, or may decay, yielding astrophysical signals. Last, we present a model with light hidden pions that may be tested with improved constraints on the number of nonrelativistic degrees of freedom. All of these scenarios are defined by a small number of parameters, are consistent with gauge coupling unification, preserve the beautiful connection between the weak scale and the observed dark matter relic density, and are natural, with relatively light visible superpartners. We conclude with comments on interesting future directions.

Highlights

  • S WIMPless anomaly-mediated supersymmetry breaking (AMSB) models with non-Abelian hidden sectors and highlight unusual possibilities that V I emerge in even the simplest models

  • If the hidden sector is localized on the same brane as the minimal supersymmetric standard model (MSSM), it is likewise sequestered from the SUSY breaking

  • The scale of the hidden LSP (hLSP) mass mX, we are left with a non-supersymmetric SU(N ) gauge theory with NF flavors

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Summary

Visible Sector

In AMSB models the soft SUSY-breaking masses are determined by the gravitino mass m3/2 and the values of the dimensionless couplings of the theory at the SUSY-breaking scale. If the hidden sector is localized on the same brane as the MSSM, it is likewise sequestered from the SUSY breaking. Sequestering results if the SUSY-breaking sector is near-conformal over some energy range [26]. In this case, not just the MSSM, but any other sector of the theory is sequestered from the SUSY breaking, so no extra assumptions are needed regarding the dark matter hidden sector

Hidden Sector
COSMOLOGICAL CONSTRAINTS AND RELIC DENSITIES
Relic Density of Visible LSPs
Relic Density of Hidden LSPs
Relic Density of Hidden Quark-Gluon Composites
Connectors
Decay Lifetimes
Viable Scenarios
Hidden Glueballs Decaying Before BBN
Findings
VIII. CONCLUSIONS
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