Implications of Recent Nucleon Spin Structure Measurements for Neutralino Dark Matter Detection (original) (raw)
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Neutrino fluxes could arise due to annihilation of Weakly Interactive Massive Particles (WIMPs) in the center of the sun. We study the prospects of search for muon events due to such neutrinos at the upcoming Iron CALorimeter (ICAL) detector to be housed at Indiabased Neutrino Observatory (INO). Although the atmospheric neutrinos will pose a serious background to the signal neutrinos produced through WIMP annihilation, the former could be supressed significantly by using the directional property of signal neutrinos. For 50kt × 10 years of ICAL running and WIMP masses (mχ) between 3-100 GeV, we perform a χ 2 analysis and present expected exclusion regions in the σ SD − m χ and σ SI − m χ plane, where σ SD and σSI are the WIMP-nucleon Spin-Dependent (SD) and Spin-Independent (SI) scattering crosssections, respectively. For m χ = 25 GeV, the expected 90 % C.L. exclusion limit on σ SD are σSD < 7.82 × 10 −41 cm 2 for τ + τ − channel and σSD < 1.23 × 10 −39 cm 2 for bb channel. For same m χ , the expected 90 % C.L. exclusion limits on σ SI are σ SI < 8.97 × 10 −43 cm 2 for τ + τ − channel and σ SI < 1.43 × 10 −41 cm 2 for bb channel.
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International Journal of Modern Physics A, 2004
The existence of dark matter was suggested, using simple gravitational arguments, seventy years ago. Although we are now convinced that most of the mass in the Universe is indeed some nonluminous matter, we still do not know its composition. The problem of the dark matter in the Universe is reviewed here. Particle candidates for dark matter are discussed with particular emphasis on Weakly Interacting Massive Particles (WIMP's). Experiments searching for these relic particles, carried out by many groups around the world, are also reviewed, paying special attention to their direct detection by observing the elastic scattering on target nuclei through nuclear recoils. Finally, we concentrate on the theoretical models predicting WIMP's, and in particular on supersymmetric extensions of the standard model, where the leading candidate for WIMP, the neutralino, is present. There, we compute the cross-section for the direct detection of neutralinos, and compare it with the sensitivi...
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Beginning with a set of simplified models for spin-0, spin-$\half$, and spin-1 dark matter candidates using completely general Lorentz invariant and renormalizable Lagrangians, we derive the full set of non-relativistic operators and nuclear matrix elements relevant for direct detection of dark matter, and use these to calculate rates and recoil spectra for scattering on various target nuclei. This allows us to explore what high energy physics constraints might be obtainable from direct detection experiments, what degeneracies exist, which operators are ubiquitous and which are unlikely or sub-dominant. We find that there are operators which are common to all spins as well operators which are unique to spin-$\half$ and spin-1 and elucidate two new operators which have not been previously considered. In addition we demonstrate how recoil energy spectra can distinguish fundamental microphysics if multiple target nuclei are used. Our work provides a complete roadmap for taking generic ...
General analysis of direct dark matter detection: From microphysics to observational signatures
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Beginning with a set of simplified models for spin-0, spin-1 2 , and spin-1 dark matter candidates using completely general Lorentz invariant and renormalizable Lagrangians, we derive the full set of non-relativistic operators and nuclear matrix elements relevant for direct detection of dark matter, and use these to calculate rates and recoil spectra for scattering on various target nuclei. This allows us to explore what high energy physics constraints might be obtainable from direct detection experiments, what degeneracies exist, which operators are ubiquitous and which are unlikely or subdominant. We find that there are operators which are common to all spins as well operators which are unique to spin-1 2 and spin-1 and elucidate two new operators which have not been previously considered. In addition we demonstrate how recoil energy spectra can distinguish fundamental microphysics if multiple target nuclei are used. Our work provides a complete roadmap for taking generic fundamental dark matter theories and calculating rates in direct detection experiments. This provides a useful guide for experimentalists designing experiments and theorists developing new dark matter models.
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We consider the neutralino proton cross section for detection of Milky Way dark matter for a number of supergravity models with gauge unification at the GUT scale: models with universal soft breaking (mSUGRA), models with nonuniversal soft breaking, and string inspired D-brane models. The parameter space examined includes m 1/2 <1 TeV and tan β < 50, and the recent Higgs bound of m h >114 GeV is imposed. (For grand unified models, this bound is to be imposed for all tan β.) All coannihilation effects are included as well as the recent NLO corrections to b → sγ for large tan β, and coannihilation effects are shown to be sensitive to A 0 for large tan β. In all models, current detectors are sampling parts of the paramater space i. e. tan β > ∼ 25 for mSUGRA, tan β > ∼ 7 for nonuniversal models, and tan β > ∼ 20 for D-brane models. Future detectors should be able to cover almost the full parameter space for µ > 0. For µ < 0, cancellations can occur for m 1/2 > ∼ 450 GeV, allowing the cross sections to become < ∼ 10 −10 pb for limited ranges of tan β. (The positions of these cancellations are seen to be sensitive to the value of σ πN .) In this case, the gluino and squarks lie above 1 TeV, but still should be accessible to the LHC if m 1/2 < 1 TeV.
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