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 [2017/10/11 23:46] jonathan.butterworth |
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| {{:2017:groups:tools:cl_78wzg_nso.png?200|}} $(l^+l^-)$ or $(l + E_T^{\rm miss}) + \gamma$ | {{:2017:groups:tools:cl_78wzg_nso.png?200|}} $(l^+l^-)$ or $(l + E_T^{\rm miss}) + \gamma$ | ||
| - | {{:2017:groups:tools:cl_8metg_nso.png?200|}} $E_T^{\rm miss} + \gamma$ | + | {{:2017:groups:tools:cl_8metg_nso.png?200|}} $E_T^{\rm miss} + \gamma (\gamma$ |
| {{:2017:groups:tools:cl_78photons_nso.png?200|}} Inclusive and di-photons | {{:2017:groups:tools:cl_78photons_nso.png?200|}} Inclusive and di-photons | ||
| Line 64: | Line 64: | ||
| == $M_\phi = 80$ 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== | ||
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| Note that the sensitivity at low $M_\phi$ and $\Lambda$ is somewhat reduced, especially for the $E_T^{\rm miss} + \gamma$ channel. Presumably something to do with the angular distributions of the decay photons of the $\phi$, but to be studied... | Note that the sensitivity at low $M_\phi$ and $\Lambda$ is somewhat reduced, especially for the $E_T^{\rm miss} + \gamma$ channel. Presumably something to do with the angular distributions of the decay photons of the $\phi$, but to be studied... | ||
| + | |||
| + | There is still 95% exclusion even at the highest $\Lambda$ values studied. Would be interesting to see how far it goes. Update - not very far? Here's an 8 TeV run going to higher values. | ||
| + | |||
| + | {{:2017:groups:tools:cl_8extended.png?300|}}{{:2017:groups:tools:contur_8tev-cpe-extended.png?300|}} | ||
2017/groups/tools/contur_for_light_scalar_particles.txt ยท Last modified: 2017/10/11 23:47 by jonathan.butterworth
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