Supersymmetry After the Higgs Discovery 2014
DOI: 10.1007/978-3-662-44172-5_7
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SUSY dark matter(s)

Abstract: We review here the status of different dark matter candidates in the context of supersymmetric models, in particular the neutralino as a realization of the WIMP-mechanism and the gravitino. We give a summary of the recent bounds in direct and indirect detection and also of the LHC searches relevant for the dark matter question. We discuss also the implications of the Higgs discovery for the supersymmetric dark matter models and give the prospects for the future years. .Pb Supersymmetry PACS

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Cited by 10 publications
(18 citation statements)
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“…However, it was shown in [136] that the Zb LbL vertex can be protected from large corrections by a P LR parity symmetry, as long as the b L embedding does not break it, that is, if b L has −1/2 charge under both SU(2) L and SU(2) R . 13 As for the custodial symmetry, when this custodial parity is preserved by the strong sector, corrections to Zb LbL can be kept under control. Both symmetries yield important consequences for the quantum numbers and spectrum of the top partner resonances (for instance extended representations such as the 4 = (2, 2)).…”
Section: Non-universalmentioning
confidence: 99%
See 3 more Smart Citations
“…However, it was shown in [136] that the Zb LbL vertex can be protected from large corrections by a P LR parity symmetry, as long as the b L embedding does not break it, that is, if b L has −1/2 charge under both SU(2) L and SU(2) R . 13 As for the custodial symmetry, when this custodial parity is preserved by the strong sector, corrections to Zb LbL can be kept under control. Both symmetries yield important consequences for the quantum numbers and spectrum of the top partner resonances (for instance extended representations such as the 4 = (2, 2)).…”
Section: Non-universalmentioning
confidence: 99%
“…Both symmetries yield important consequences for the quantum numbers and spectrum of the top partner resonances (for instance extended representations such as the 4 = (2, 2)). Figure 3 reproduced from [137] shows the best fit region with a small positive δg Rb where the following parametrization is used: 14 13 Notice that in symmetry breaking cosets with unbroken SO(4), P LR actually arises as an accidental symmetry of the leading order derivative Lagrangian [96]. 14 There exists another best fit region with a larger negative δg Rb .…”
Section: Non-universalmentioning
confidence: 99%
See 2 more Smart Citations
“…This is often referred to as the gravitino problem in cosmology [1,2]. Of course the other possibility is for the gravitinos to be the lightest supersymmetric particle and in that case they can also successfully play the role of Dark Matter [3][4][5][6][7]. We are here instead interested in a different scenario, where the gravitinos are ultra-light, with masses much smaller than the electroweak scale or even the other SM particle masses.…”
Section: Introductionmentioning
confidence: 99%