2008
DOI: 10.1016/j.asr.2007.02.067
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Status and perspectives of indirect and direct dark matter searches

Abstract: In this review article the current status of particle dark matter is addressed. We discuss the main theoretical extensions of the standard model which allow to explain dark matter in terms of a (yet undiscovered) elementary particle. We then discuss the theoretical predictions for the searches of particle dark matter: direct detection in low background underground experiments and indirect detection of neutrinos, gamma-rays and antimatter with terrestrial and space-borne detectors. Attention will be placed also… Show more

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Cited by 8 publications
(8 citation statements)
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“…μν is symmetric and divergence-free (∇ μ T (N ) μν = 0) in agreement with (6). In the Newtonian regime thus T (N ) μν qualifies as the well-known conserved energy-momentum tensor of matter…”
Section: Modified Energeticssupporting
confidence: 52%
See 1 more Smart Citation
“…μν is symmetric and divergence-free (∇ μ T (N ) μν = 0) in agreement with (6). In the Newtonian regime thus T (N ) μν qualifies as the well-known conserved energy-momentum tensor of matter…”
Section: Modified Energeticssupporting
confidence: 52%
“…The DM hypothesis provides viable explanations not only for flat rotation curves but also for various cosmological and astronomical observations describing different phases of the evolution of the Universe. Several experimental groups have been searching for DM particles by utilizing various detection methods (see the recent review volumes [5,6]). So far, no signal of DM has been observed.…”
Section: Introductionmentioning
confidence: 99%
“…From the experimental point of view, direct and indirect methods [130] exist for detecting the WIMPs in the galactic halo. The methods can probe complementary regions of the supersymmetric parameter space, even when more extensive LHC results will become available.…”
Section: Indirect Dark Matter Searchesmentioning
confidence: 99%
“…28) where W T,P = c W c T,P , W c T,P = (σ c T,P θ c fwhm ) −2 is the weight per solid angle for temperature and polarisation respectively, with a 1-σ sensitivity per pixel of σ c T,P and a beam of θ c fwhm extent, for each frequency channel c. The beam window function is given in terms of the full width half maximum (fwhm) beam width by B 2 ℓ…”
mentioning
confidence: 99%