CERN Accelerating science

 
Profile likelihood ratios of the Higgs decay constant $f$ in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$. For reference, the best-fit points found in these models have respective negative log likelihoods of $15.3$, $15.1$, and $15.4$.
Profile likelihood ratios of the Higgs decay constant $f$ in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$. For reference, the best-fit points found in these models have respective negative log likelihoods of $15.3$, $15.1$, and $15.4$.
Profile likelihood ratios of the Higgs decay constant $f$ in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$. For reference, the best-fit points found in these models have respective negative log likelihoods of $15.3$, $15.1$, and $15.4$.
Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
Profile likelihood ratios of the masses of the lightest up-type (U) and down-type (D) composite resonances in (a) the M4DCHM$^{5-5-5}$, (b) the M4DCHM$^{14-14-10}$, (c) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.
Cross sections for the pair-production of the lightest up-type (U) and down-type (D) resonances decaying into various final states at the $\sqrt{s}=13$~TeV LHC for viable points in (top) the M4DCHM$^{5-5-5}$, (middle) the M4DCHM$^{14-14-10}$, (bottom) the M4DCHM$^{14-1-10}$.