Abstract

We explore the potential of the ${e}^{+}{e}^{\ensuremath{-}}$ colliders to discover dark matter and determine its properties such as mass and spin. For this purpose we study spin zero and spin one-half cases of dark matter $D$, which belongs to the $SU(2)$ weak doublet and therefore has the charged doublet partner ${D}^{+}$. For the case of scalar dark matter we chose inert doublet model, while for the case of fermion dark matter we suggest the new minimal fermion dark matter model with only three parameters. We choose two benchmarks for the models under study, which provide the correct amount of observed dark matter (DM) relic density and consistent with the current DM searches. We focus on the particular process ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}^{+}{D}^{\ensuremath{-}}\ensuremath{\rightarrow}DD{W}^{+}{W}^{\ensuremath{-}}\ensuremath{\rightarrow}DD(q\overline{q})({\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\nu})$ at the 500 GeV ILC collider that gives rise to the ``$\mathrm{dijet}+\ensuremath{\mu}+{\overline{)E}}_{T}$'' signature and study it at the level of fast detector simulation, taking into account bremsstrahlung and ISR effects. We have found that two kinematical observables---the energy of the muon ${E}_{\ensuremath{\mu}}$ and the angular distribution of the $W$ boson, reconstructed from dijet $\mathrm{cos}{\ensuremath{\theta}}_{jj}$ are very powerful in determination of DM mass and spin, respectively. In particular we have demonstrated that in the case of fermion DM, the masses can be measured with a few percent accuracy already at $500\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ integrated luminosity. At the same time, the scalar DM model which has about an order of magnitude lower signal, requires about a factor of 40 higher luminosity to reach the same accuracy in the mass measurement. We have found that one can distinguish fermion and scalar DM scenarios with about $2\text{ }\text{ }{\mathrm{ab}}^{\ensuremath{-}1}$ total integrated luminosity or less without using the information on the cross sections for benchmarks under study. The methods of the determination of DM properties which we suggest here are generic for the models where DM and its partner belong to the weak multiplet and can be applied to explore various DM models at future ${e}^{+}{e}^{\ensuremath{-}}$ colliders.

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