First search for dyons with the full MoEDAL trapping detector in 13 TeV pp collisions
- Acharya, B. et al
- arXiv:2002.00861
 | Feynman-like diagram for dyon-pair direct production at leading order via the benchmark Drell-Yan mechanism. The coupling $g'$ is given by $\sqrt{(g^{2} + q^{2})}$, in the eikonal approximation that is valid for LHC energies. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY spin-0, 1/2 and 1 dyon-pair production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY spin-0, 1/2 and 1 dyon-pair production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 1$g_{D}$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading-order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 2$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 3$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 4$\gd$ and multiple electric charges, in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |
 | Cross-section upper limits at 95\% CL for DY dyon pair-production, with magnetic charge 5$g_{D}$ and 6$g_{D}$ and multiple electric charges in 13~\tev $pp$ collisions as a function of spin. The solid lines are leading order cross-section calculations. |