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2017:groups:tools:contur [2017/09/20 23:03] jonathan.butterworth |
2017:groups:tools:contur [2017/09/21 10:24] jonathan.butterworth |
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* [[contur#2HDM Studies|2HDM Studies]] | * [[contur#2HDM Studies|2HDM Studies]] | ||
* [[2017:groups:higgs:fxsnp:susycascades|FXS: Higgs production from SUSY cascades]] | * [[2017:groups:higgs:fxsnp:susycascades|FXS: Higgs production from SUSY cascades]] | ||
- | * [[contur#Light Scalar Particles|Light Scalar Particles]] | + | * [[Contur for Light Scalar Particles]] |
* [[Explanation of Contur plot format]] | * [[Explanation of Contur plot format]] | ||
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For each case, all the other f's should be set to very large values. | For each case, all the other f's should be set to very large values. | ||
+ | So, here is a scan using these ranges for the CP-odd scalar model (f0 value labelled $\Lambda$ on the vertical axis, $M_\phi$ on the horizontal. | ||
+ | {{2017:groups:tools:colorbarkey.png}} | ||
+ | |||
+ | {{:2017:groups:tools:combinedcl_.png?400|}} | ||
+ | |||
+ | ... so this is looking pretty promising. Everything excluded except the lowest mass/highest scale. This needs to be carefully checked, of course. All the yellow region above is excluded by the ATLAS diphoton cross sections: [[http://inspirehep.net/record/1591327|arXiv:1704.03839]]. If those are not included, the [[http://inspirehep.net/record/1448301|ATLAS $Z+\gamma$ measurements]] (in dilepton+photon and MET+photon) have quite some power on their own, see below. | ||
+ | |||
+ | {{:2017:groups:tools:combinedcl_zg.png?400|}} | ||
+ | Z+photon | ||
+ | |||
+ | {{:2017:groups:tools:combinedcl_metg.png?400|}} | ||
+ | Missing ET + photon | ||
+ | |||
+ | Remember, big caveat on this is that the data is assumed to exactly agree with the SM, which means (given we only really know that these data are //consistent// with the SM) that we are neglected the SM theory uncertainties. | ||
== Older Stuff == | == Older Stuff == |