2010
DOI: 10.1103/physrevd.81.095017
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Multicomponent dark matter in supersymmetric hidden sector extensions

Abstract: Most analyses of dark matter within supersymmetry assume the entire cold dark matter arising only from weakly interacting neutralinos. We study a new class of models consisting of U(1) n hidden sector extensions of the minimal supersymmetric standard model that includes several stable particles, both fermionic and bosonic, which can be interpreted as constituents of dark matter. In one such class of models, dark matter is made up of both a Majorana dark matter particle, i.e., a neutralino, and a Dirac fermion … Show more

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Cited by 112 publications
(119 citation statements)
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References 156 publications
(141 reference statements)
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“…Now in the leptonic sector it is known [22] that for the standard model case we may choose one of the linear combinations L e − L µ , L µ − L τ , L e − L τ to be anomaly free and can be gauged. The gauged L e − L µ has been discussed previously in the context of PAMELA positron excess and multi-component dark matter [8] and L µ − L τ in the context of muon anomalous moment [23] and in the context the PAMELA positron excess [24]. Here we consider a gauged L µ − L τ in the discussion of asymmetric dark matter as this choice is the more appropriate one for the analysis here.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Now in the leptonic sector it is known [22] that for the standard model case we may choose one of the linear combinations L e − L µ , L µ − L τ , L e − L τ to be anomaly free and can be gauged. The gauged L e − L µ has been discussed previously in the context of PAMELA positron excess and multi-component dark matter [8] and L µ − L τ in the context of muon anomalous moment [23] and in the context the PAMELA positron excess [24]. Here we consider a gauged L µ − L τ in the discussion of asymmetric dark matter as this choice is the more appropriate one for the analysis here.…”
Section: Introductionmentioning
confidence: 99%
“…In this manuscript we analyze this issue in the framework of a Stueckelberg U (1) extension of the standard model (SM) as well as a Stueckelberg U (1) extension of the minimal supersymmetric standard model (MSSM) [3][4][5][6][7][8][9]. There are two main constraints in building models with asymmetric dark matter (AsyDM).…”
Section: Introductionmentioning
confidence: 99%
“…We define (Ω χ h 2 ) WMAP ≡ 0.1120, the central value from the WMAP-7 data. Only taking the WMAP upper limit allows for the possibility of multicomponent dark matter [46]. Other constraints applied to the mSUGRA parameter points include the g µ − 2 [47] constraint −11.4 × 10 −10 ≤ δ (g µ − 2) ≤ 9.4 × 10 −9 and constraints from B-physics measurements [48][49][50] which yield flavor constraints from the data, i.e.…”
Section: Higgs Mass In Minimal Sugramentioning
confidence: 99%
“…We recall that Stückelberg fields appear both in anomalous and in non-anomalous contexts. The second one has been analyzed recently in [54].…”
Section: A General Features Of the Modelmentioning
confidence: 99%