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Higgs Sector of Non-minimal Supersymmetric Models at Future Hadron Colliders - Hugonie, Cyril et al - hep-ph/0110241RAL-TR-2001-036CERN-TH-2001-241IPPP-01-46SNOWMASS-2001-P108
 
Total number of events produced through processes (\ref{procs}) at the Tevatron (Run II) after 15 fb$^{-1}$ in the NMSSM (upper plots) and n
Total number of events produced through processes (\ref{procs}) at the Tevatron (Run II) after 15 fb$^{-1}$ in the NMSSM (upper plots) and n
Total number of events produced through processes (\ref{procs}) at the Tevatron (Run II) after 15 fb$^{-1}$ in the NMSSM (upper plots) and n
Total number of events produced through processes (\ref{procs}) at the Tevatron (Run II) after 15 fb$^{-1}$ in the NMSSM (upper plots) and n
As Fig.~\ref{fig:Tevatron} for the CP-even singlet $S_r$ (left plots) and the CP-odd singlet $S_i$ (right plots), at LHC after 300 fb$^{-1}$
As Fig.~\ref{fig:Tevatron} for the CP-even singlet $S_r$ (left plots) and the CP-odd singlet $S_i$ (right plots), at LHC after 300 fb$^{-1}$
As Fig.~\ref{fig:Tevatron} for the CP-even singlet $S_r$ (left plots) and the CP-odd singlet $S_i$ (right plots), at LHC after 300 fb$^{-1}$
As Fig.~\ref{fig:Tevatron} for the CP-even singlet $S_r$ (left plots) and the CP-odd singlet $S_i$ (right plots), at LHC after 300 fb$^{-1}$