2014
DOI: 10.1103/physrevd.89.103528
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Constraints on light magnetic dipole dark matter from the ILC and SN 1987A

Abstract: To illustrate the complementarity of the linear collider and astrophysics bounds on the light (MeV-scale mass) dark matter (DM), we study the constraints on the magnetic dipole DM from the DM-electron interactions at the proposed International Linear Collider (ILC) and in supernova (SN) 1987A. We in particular focus on the e þ e − annihilation, which is the common process for producing DM pairs both at the ILC and in the SN. We estimate the bounds on the DM magnetic dipole moment from the monophoton signals at… Show more

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Cited by 25 publications
(22 citation statements)
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References 89 publications
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“…We note that while the analysis of ref. [95] does not include Pauli blocking effects, the above bound converts into an effective suppression scale of the dimension-five dipole operator of order ∼ 10 9 GeV, which is comparable to the constraint on the suppression scale of the axion-photon coupling from supernova cooling considerations [69]. We thus believe the order of magnitude of the constraint is valid.…”
Section: Dipole Operator Dark Mattermentioning
confidence: 61%
“…We note that while the analysis of ref. [95] does not include Pauli blocking effects, the above bound converts into an effective suppression scale of the dimension-five dipole operator of order ∼ 10 9 GeV, which is comparable to the constraint on the suppression scale of the axion-photon coupling from supernova cooling considerations [69]. We thus believe the order of magnitude of the constraint is valid.…”
Section: Dipole Operator Dark Mattermentioning
confidence: 61%
“…10 and 11. While the bounds above are stronger than those derived from LHC data [82,83], future experiments, such as ILC and HL-LHC, may improve the sensitivity on these couplings by one to two orders of magnitude [84][85][86].…”
Section: F Missing Energy At High-energy Collidersmentioning
confidence: 76%
“…Our specific example, the velocity-dependent elastic scattering cross-section, would be also of great interest for particle physics studies because of its infrared enhancement for a low momentum transfer, which has been explored for potential signals beyond the standard model at collider and dark matter search experiments [21,23,24,25,26]. Such probes of the dark matter properties from both cosmology and particle physics deserve further study in view of forthcoming experiments which can explore the nature of the DM coupling to ordinary baryons.…”
Section: Discussionmentioning
confidence: 99%
“…The spectral index n depends on the nature of DM models, for instance, n = −1 corresponds to the Yukawa-type potential DM , n = −2, −4 are respectively for dipole DM and millicharged DM [3,4,5,6,20,21,22,23,24,25,26]. The constant coefficient c n depends on the value of n and also can include the correction factor for including the helium in addition to hydrogen.…”
Section: Thermal Evolution Of Baryons and Dm With Dm-baryon Couplingmentioning
confidence: 99%