Benchmark points for ggF->H3->(H_SM->bb or tautau)+(H_singlet->bb)
These benchmark points correspond to maximally possible cross sections for the above process in the NMSSM respecting constraints as implemented in NMSSMTools:
- Mass and couplings (in the kappa framework) of the SM-like Higgs scalar; the mass allows for +/- 2 GeV theoretical uncertainty
- BSM searches at the LHC, and constraints from LEP
- B-physics
- Dark matter direct detection experiments (the relic density is typically too small, allowing for additional contributions from hidden sectors)
| 900 |
62 |
0.586E-02 |
0.624E-03 |
| 900 |
80 |
0.584E-02 |
0.622E-03 |
| 900 |
100 |
0.581E-02 |
0.618E-03 |
| 900 |
120 |
0.590E-02 |
0.628E-03 |
| 900 |
125 |
0.592E-02 |
0.630E-03 |
| 900 |
130 |
0.594E-02 |
0.632E-03 |
| 900 |
150 |
0.602E-02 |
0.640E-03 |
| 900 |
200 |
0.616E-02 |
0.656E-03 |
| 900 |
300 |
0.487E-02 |
0.517E-03 |
| 900 |
400 |
0.849E-03 |
0.903E-04 |
| 900 |
500 |
0.473E-03 |
0.503E-04 |
| 900 |
600 |
0.256E-03 |
0.273E-04 |
| 1000 |
62 |
0.192E-02 |
0.204E-03 |
| 1000 |
80 |
0.191E-02 |
0.204E-03 |
| 1000 |
100 |
0.189E-02 |
0.201E-03 |
| 1000 |
120 |
0.194E-02 |
0.206E-03 |
| 1000 |
130 |
0.201E-02 |
0.215E-03 |
| 1000 |
150 |
0.207E-02 |
0.220E-03 |
| 1000 |
200 |
0.217E-02 |
0.231E-03 |
| 1000 |
300 |
0.135E-02 |
0.143E-03 |
| 1000 |
400 |
0.342E-03 |
0.364E-04 |
| 1000 |
500 |
0.172E-03 |
0.183E-04 |
| 1000 |
600 |
0.132E-03 |
0.140E-04 |
| 1200 |
62 |
0.516E-03 |
0.550E-04 |
| 1200 |
80 |
0.513E-03 |
0.546E-04 |
| 1200 |
100 |
0.504E-03 |
0.536E-04 |
| 1200 |
150 |
0.492E-03 |
0.527E-04 |
| 1200 |
200 |
0.547E-03 |
0.582E-04 |
| 1200 |
300 |
0.447E-03 |
0.475E-04 |
| 1200 |
400 |
0.110E-03 |
0.117E-04 |
| 1200 |
500 |
0.564E-04 |
0.600E-05 |
| 1200 |
600 |
0.422E-04 |
0.449E-05 |
| 1400 |
62 |
0.161E-03 |
0.171E-04 |
| 1400 |
80 |
0.168E-03 |
0.179E-04 |
| 1400 |
100 |
0.154E-03 |
0.165E-04 |
| 1400 |
120 |
0.153E-03 |
0.163E-04 |
| 1400 |
130 |
0.152E-03 |
0.163E-04 |
| 1400 |
150 |
0.156E-03 |
0.166E-04 |
| 1400 |
200 |
0.140E-03 |
0.149E-04 |
| 1400 |
300 |
0.129E-03 |
0.137E-04 |
| 1400 |
400 |
0.410E-04 |
0.436E-05 |
| 1400 |
500 |
0.214E-04 |
0.228E-05 |
| 1400 |
600 |
0.161E-04 |
0.171E-05 |
| 1600 |
62 |
0.480E-04 |
0.512E-05 |
| 1600 |
80 |
0.473E-04 |
0.504E-05 |
| 1600 |
100 |
0.439E-04 |
0.467E-05 |
| 1600 |
150 |
0.432E-04 |
0.459E-05 |
| 1600 |
200 |
0.448E-04 |
0.477E-05 |
| 1600 |
300 |
0.312E-04 |
0.331E-05 |
| 1600 |
400 |
0.128E-04 |
0.136E-05 |
| 1600 |
500 |
0.639E-05 |
0.679E-06 |
| 1600 |
600 |
0.469E-05 |
0.499E-06 |
| 1800 |
62 |
0.169E-04 |
0.180E-05 |
| 1800 |
80 |
0.168E-04 |
0.179E-05 |
| 1800 |
100 |
0.165E-04 |
0.176E-05 |
| 1800 |
150 |
0.150E-04 |
0.160E-05 |
| 1800 |
200 |
0.154E-04 |
0.164E-05 |
| 1800 |
300 |
0.820E-05 |
0.872E-06 |
| 1800 |
400 |
0.469E-05 |
0.498E-06 |
| 1800 |
500 |
0.254E-05 |
0.270E-06 |
| 1800 |
600 |
0.187E-05 |
0.199E-06 |
| 2000 |
62 |
0.661E-05 |
0.703E-06 |
| 2000 |
80 |
0.659E-05 |
0.700E-06 |
| 2000 |
100 |
0.662E-05 |
0.704E-06 |
| 2000 |
150 |
0.653E-05 |
0.695E-06 |
| 2000 |
200 |
0.637E-05 |
0.678E-06 |
| 2000 |
300 |
0.283E-05 |
0.301E-06 |
| 2000 |
400 |
0.191E-05 |
0.203E-06 |
| 2000 |
500 |
0.123E-05 |
0.130E-06 |
| 2000 |
600 |
0.106E-05 |
0.113E-06 |
| 2500 |
62 |
0.555E-06 |
0.591E-07 |
| 2500 |
80 |
0.587E-06 |
0.625E-07 |
| 2500 |
100 |
0.594E-06 |
0.632E-07 |
| 2500 |
150 |
0.613E-06 |
0.653E-07 |
| 2500 |
200 |
0.664E-06 |
0.707E-07 |
| 2500 |
300 |
0.524E-06 |
0.558E-07 |
| 2500 |
400 |
0.384E-06 |
0.408E-07 |
| 2500 |
500 |
0.235E-06 |
0.250E-07 |
| 2500 |
600 |
0.179E-06 |
0.190E-07 |
| 3000 |
150 |
0.404E-07 |
0.430E-08 |
| 3000 |
200 |
0.238E-07 |
0.254E-08 |
png 
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