Hunting magnetic monopoles and more with MoEDAL at the LHC
- Mitsou, Vasiliki A.
- arXiv:1710.08609DESY-PROC-2017-02/mitsou_vasilikiPUBDB-2018-01768
 | A three-dimensional schematic view of the MoEDAL detector (in the yellow circle) around the LHCb VELO region at Point~8 of the LHC. |
 | A three-dimensional schematic view of the MoEDAL detector (in the yellow circle) around the LHCb VELO region at Point~8 of the LHC. |
 | Left: Cross-section upper limits at 95\% C.L.\ for DY monopole production as a function of mass for spin-1/2 monopoles~\cite{MMT13TeV}. Right: Excluded monopole masses for DY production for spin-$1/2$ (top) and spin-$0$ (bottom) monopoles. The MoEDAL results obtained at 8~TeV~\cite{MMT8TeV} and 13~TeV~\cite{MMT13TeV} are superimposed on the ATLAS 8-TeV limits~\cite{atlas8tev}. |
 | Left: Cross-section upper limits at 95\% C.L.\ for DY monopole production as a function of mass for spin-1/2 monopoles~\cite{MMT13TeV}. Right: Excluded monopole masses for DY production for spin-$1/2$ (top) and spin-$0$ (bottom) monopoles. The MoEDAL results obtained at 8~TeV~\cite{MMT8TeV} and 13~TeV~\cite{MMT13TeV} are superimposed on the ATLAS 8-TeV limits~\cite{atlas8tev}. |
 | Left: Cross-section upper limits at 95\% C.L.\ for DY monopole production as a function of mass for spin-1/2 monopoles~\cite{MMT13TeV}. Right: Excluded monopole masses for DY production for spin-$1/2$ (top) and spin-$0$ (bottom) monopoles. The MoEDAL results obtained at 8~TeV~\cite{MMT8TeV} and 13~TeV~\cite{MMT13TeV} are superimposed on the ATLAS 8-TeV limits~\cite{atlas8tev}. |
 | Left: Cross-section upper limits at 95\% C.L.\ for DY monopole production as a function of mass for spin-1/2 monopoles~\cite{MMT13TeV}. Right: Excluded monopole masses for DY production for spin-$1/2$ (top) and spin-$0$ (bottom) monopoles. The MoEDAL results obtained at 8~TeV~\cite{MMT8TeV} and 13~TeV~\cite{MMT13TeV} are superimposed on the ATLAS 8-TeV limits~\cite{atlas8tev}. |