For S 500 Gev And M H 130 Gev We Plot Sm As A Function
For √ s = 500 GeV and M H = 130 GeV , we plot |∆σ/σ SM | as a function ...
For √ s = 500 GeV and M H = 130 GeV , we plot |∆σ/σ SM | as a function ...
The relative correction δσ/σ SM as a function of M Z at √ s = 500 GeV ...
We plot Re a1,2(s) for m h = 870 GeV, m φ = 500 GeV and Λ = Λ φ = 5 TeV ...
We plot Re a1,2(s) for m h = 870 GeV, m φ = 500 GeV and Λ = Λ φ = 5 TeV ...
We plot Re a0,1,2(s) for m h = 870 GeV, m φ = 500 GeV and Λ = Λ φ = 5 ...
We plot Re a1,2(s) for m h = 870 GeV, m φ = 500 GeV and Λ = Λ φ = 5 TeV ...
Light Higgs mass M h in GeV as a function of M A in GeV and tan β for ...
M h (left) and M S (right) as a function of a S H . m tree S = 1000 ...
m h is plotted versus m L keeping M R = 500 GeV and A N = 0 . The stop ...
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M h (left) and M S (right) as a function of a S H . m tree S = 1000 ...
Obtained experimental bound on f W and f W W for M H = 500 GeV heavy ...
The SM prediction for M W as a function of M H for m t = 174.3 ± 5.1 ...
The same as fig. 5 but for the different point m 1 / 2 = 500 GeV and m ...
b → sγ constraint. We use the parameter set in (23) and m H ± = 130 GeV ...
M h,H,H ± vary with respect to M A for M ˜ t = 500 GeV, A t = −740 GeV ...
Signal cross sections for m H ± = 200 GeV, tan β = 5, and √ s = 500 ...
The cross section σ(s) as a function of the mass parameter M W H for M ...
Allowed parameter space in the (λ φS ,λ Hφ ) plane for m S = 500 GeV ...
Computing the optimal weight function to select a 2 at √ s = 500 GeV ...
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Discovery limits in the (m N , U 2 eN )-plane for √ s = 500 GeV and ...
Total cross section for e + e − → h ˜ χ + 1 ˜ χ − 1 at √ s = 500 GeV ...
Signal and background rates for L = 50 fb −1 at √ s = 500 GeV for e + e ...
Computing the optimal weight function to select a 2 at √ s = 500 GeV ...
As for Fig. 8, with m 3/2 = 500 GeV but unchanged values for the CMSSM ...
Relative difference between pressure at m H = 130 GeV and m H = 200 GeV ...
Total cross section for ͑ left plot ͒ e ϩ e Ϫ → ZH i at ͱ s ϭ 500 GeV ...
Plots of ∆T versus M S 2 with (a) M H = 60 GeV and (b) M H = 70 GeV ...
Same plot as in Fig. 7 but with a DM particle mass of 500 GeV ...
Contours of the process pp → A → γγ for the two values m A = 500 GeV ...
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Relative difference between pressure at m H = 130 GeV and m H = 200 GeV ...
Total cross section for e + e − → h ˜ χ + 1 ˜ χ − 1 at √ s = 500 GeV ...
For m χ ± 1 = 175 GeV, √ s = 600 GeV and central values of ∆m˜χ∆m˜ ∆m˜χ ...
Br inv-dependence of γγ R for (a) M = 150 GeV and 500 GeV ⩽ ⩽ f 1500 ...
Same of Fig. 4 for √ s = 500 GeV and L = 500 f b −1 . | Download ...
The branching fraction B(H1→γγ) as a function of Φ for mH1=80 GeV ...