2017:groups:tools:contur_for_light_scalar_particles
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2017:groups:tools:contur_for_light_scalar_particles [2017/10/01 11:27] jonathan.butterworth |
2017:groups:tools:contur_for_light_scalar_particles [2017/10/01 11:27] jonathan.butterworth |
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| == $M_\phi = 80$ GeV, $\Lambda = 7.5$ TeV == | == $M_\phi = 80$ GeV, $\Lambda = 7.5$ TeV == | ||
| - | > [[http://www.hep.ucl.ac.uk/~jmb/Work/LH/NSCPO/8TeV/mP_80_f0_7500/contur-plots/|Page of plots]]: This point is chosen to look at the higher end of the $M_\phi$ range, where the sensitivity is greater, and so we look at a high $\Lambda$ value. Again the sensitivity is driven by [[http://www.hep.ucl.ac.uk/~jmb/Work/LH/NSCPO/8TeV/mP_80_f0_7500/contur-plots/ATLAS_2016_I1448301_NU/index.html|this paper]], but now it is the $\gamma\gamma + E_T^{\rm miss}$ cross section that does the work. | + | > [[http://www.hep.ucl.ac.uk/~jmb/Work/LH/NSCPO/8TeV/mP_80_f0_7500/contur-plots/|Page of plots]]: This point is chosen to look at the higher end of the $M_\phi$ range, where the sensitivity is greater, and so we look at a high $\Lambda$ value. Again the sensitivity is driven by [[http://www.hep.ucl.ac.uk/~jmb/Work/LH/NSCPO/8TeV/mP_80_f0_7500/contur-plots/ATLAS_2016_I1448301_NU/index.html|this paper]], but now it is the $\gamma\gamma + E_T^{\rm miss}$ cross section that does the work. And again once the 7 TeV data are included, the inclusive and diphotons cover this point on their own. |
| == CP-even results== | == CP-even results== | ||
2017/groups/tools/contur_for_light_scalar_particles.txt ยท Last modified: 2017/10/11 23:47 by jonathan.butterworth
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