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      Singlet-Doublet model: dark matter searches and LHC constraints

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      Journal of High Energy Physics
      Springer Nature America, Inc

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          Most cited references43

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          Is Open Access

          Supersymmetric Dark Matter

          There is almost universal agreement among astronomers that most of the mass in the Universe and most of the mass in the Galactic halo is dark. Many lines of reasoning suggest that the dark matter consists of some new, as yet undiscovered, weakly-interacting massive particle (WIMP). There is now a vast experimental effort being surmounted to detect WIMPS in the halo. The most promising techniques involve direct detection in low-background laboratory detectors and indirect detection through observation of energetic neutrinos from annihilation of WIMPs that have accumulated in the Sun and/or the Earth. Of the many WIMP candidates, perhaps the best motivated and certainly the most theoretically developed is the neutralino, the lightest superpartner in many supersymmetric theories. We review the minimal supersymmetric extension of the Standard Model and discuss prospects for detection of neutralino dark matter. We review in detail how to calculate the cosmological abundance of the neutralino and the event rates for both direct- and indirect-detection schemes, and we discuss astrophysical and laboratory constraints on supersymmetric models. We isolate and clarify the uncertainties from particle physics, nuclear physics, and astrophysics that enter at each step in the calculation. We briefly review other related dark-matter candidates and detection techniques.
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            Order of Magnitude Smaller Limit on the Electric Dipole Moment of the Electron

            The Standard Model (SM) of particle physics fails to explain dark matter and why matter survived annihilation with antimatter following the Big Bang. Extensions to the SM, such as weak-scale Supersymmetry, may explain one or both of these phenomena by positing the existence of new particles and interactions that are asymmetric under time-reversal (T). These theories nearly always predict a small, yet potentially measurable (\(10^{-27}\)-\(10^{-30}\) \(e\) cm) electron electric dipole moment (EDM, \(d_e\)), which is an asymmetric charge distribution along the spin (\(\vec{S}\)). The EDM is also asymmetric under T. Using the polar molecule thorium monoxide (ThO), we measure \(d_e = (-2.1 \pm 3.7_\mathrm{stat} \pm 2.5_\mathrm{syst})\times 10^{-29}\) \(e\) cm. This corresponds to an upper limit of \(|d_e| < 8.7\times 10^{-29}\) \(e\) cm with 90 percent confidence, an order of magnitude improvement in sensitivity compared to the previous best limits. Our result constrains T-violating physics at the TeV energy scale.
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              First results from the LUX dark matter experiment at the Sanford Underground Research Facility

              The Large Underground Xenon (LUX) experiment, a dual-phase xenon time-projection chamber operating at the Sanford Underground Research Facility (Lead, South Dakota), was cooled and filled in February 2013. We report results of the first WIMP search dataset, taken during the period April to August 2013, presenting the analysis of 85.3 live-days of data with a fiducial volume of 118 kg. A profile-likelihood analysis technique shows our data to be consistent with the background-only hypothesis, allowing 90% confidence limits to be set on spin-independent WIMP-nucleon elastic scattering with a minimum upper limit on the cross section of \(7.6 \times 10^{-46}\) cm\(^{2}\) at a WIMP mass of 33 GeV/c\(^2\). We find that the LUX data are in strong disagreement with low-mass WIMP signal interpretations of the results from several recent direct detection experiments.

                Author and article information

                Journal
                Journal of High Energy Physics
                J. High Energ. Phys.
                Springer Nature America, Inc
                1029-8479
                October 2015
                October 19 2015
                October 2015
                : 2015
                : 10
                Article
                10.1007/JHEP10(2015)116
                0a8225fa-4965-4c97-9e52-7db7bd6a724d
                © 2015
                History

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