4.4 Article

Dark matter in split SUSY with intermediate higgses

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 4, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP04(2015)151

Keywords

Supersymmetry Phenomenology

Funding

  1. National Science Council of Taiwan [NSC 102-2112-M-007-015-MY3]
  2. National Research Foundation of Korea (NRF) [2013R1A2A2A01015406]
  3. Chonnam National University
  4. World Premier International Research Center Initiative (WPI), MEXT, Japan
  5. National Research Foundation of Korea [2013R1A2A2A01015406, 21A20131100008] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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The searches for heavy Higgs bosons and supersymmetric (SUSY) particles at the LHC have left the minimal supersymmetric standard model (MSSM) with an unusual spectrum of SUSY particles, namely, all squarks are beyond a few TeV while the Higgs bosons other than the one observed at 125 GeV could be relatively light. In light of this, we study a scenario characterized by two scales: the SUSY breaking scale or the squark-mass scale (MS) and the heavy Higgs-boson mass scale (MA). We perform a survey of the MSSM parameter space with M-S less than or similar to 10(10) GeV and M-A less than or similar to 10(4) GeV such that the lightest Higgs boson mass is within the range of the observed Higgs boson as well as satisfying a number of constraints. The set of constraints include the invisible decay width of the Z boson and that of the Higgs boson, the chargino-mass limit, dark matter relic abundance from Planck, the spin-independent cross section of direct detection by LUX, and gamma-ray flux from dwarf spheroidal galaxies and gamma-ray line constraints measured by Fermi LAT. Survived regions of parameter space feature the dark matter with correct relic abundance, which is achieved through either coannihilation with charginos, A/H funnels, or both. We show that future measurements, e.g., XENON1T and LZ, of spin-independent cross sections can further squeeze the parameter space.

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