2012
DOI: 10.1016/j.physletb.2012.09.036
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Dipole moment dark matter at the LHC

Abstract: Monojet and monophoton final states with large missing transverse energy ( E T ) are important for dark matter (DM) searches at colliders. We present analytic expressions for the differential cross sections for the parton-level processes, qq(qg) → g(q)χχ and qq → γχχ, for a neutral DM particle with a magnetic dipole moment (MDM) or an electric dipole moment (EDM). We collectively call such DM candidates dipole moment dark matter (DMDM). We also provide monojet cross sections for scalar, vector and axial-vector… Show more

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Cited by 44 publications
(40 citation statements)
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“…For Dirac neutrinos in BSM scenarios, naturalness considerations on the coeffecients of effective operators imply, µ ν 10 −14 µ B [31], far below present experimental sensitivity. Finally for Majorana neutrinos reactor data as measured by the GEMMA spectrometer constrains, µ ν < 3.2 × 10 −11 µ B , [32] while the 7 TeV LHC sensitivity is around ∼ 3 × 10 −5 µ B [33], far above what is allowed by reactor and solar data [34]. We conclude that neutrino magnetic moments will not produce sizeable missing energy at the LHC.…”
Section: Introductionmentioning
confidence: 77%
“…For Dirac neutrinos in BSM scenarios, naturalness considerations on the coeffecients of effective operators imply, µ ν 10 −14 µ B [31], far below present experimental sensitivity. Finally for Majorana neutrinos reactor data as measured by the GEMMA spectrometer constrains, µ ν < 3.2 × 10 −11 µ B , [32] while the 7 TeV LHC sensitivity is around ∼ 3 × 10 −5 µ B [33], far above what is allowed by reactor and solar data [34]. We conclude that neutrino magnetic moments will not produce sizeable missing energy at the LHC.…”
Section: Introductionmentioning
confidence: 77%
“…This interaction is well-motivated and arises in a wide variety of DM models [6,40,[70][71][72][73][74][75][76].…”
Section: B γ/Z-mediated Dipole Interactionmentioning
confidence: 99%
“…The processes that lead to constraints are mono-photon production (from initial or final state) plus missing energy due to the pair of DM particles in e + e − collisions at LEP, or mono-jet production plus missing energy in proton-antiproton collision in Tevatron, or proton-proton collisions at LHC. In the case of magnetic DM these constraints have been studied in [48,49] where it is found that the upper bound on λ χ is safely above the range of values of λ χ relevant for the direct search experiments (for the range of m χ ∼ 10 GeV).…”
Section: Collider and Other Astrophysical Constraintsmentioning
confidence: 99%
“…We refer to [23,[38][39][40][41][42][43][44][45][46][47][48][49][50] for a limited sample of the earlier literature.…”
Section: Introductionmentioning
confidence: 99%