Difference: Hig13005TWiki (14 vs. 15)

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Measurements of the properties of the new boson with a mass near 125 GeV

This is a condensed description with plots for the analysis CMS-PAS-HIG-13-005.
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Summary of the fits for deviations in the coupling for the generic five-parameter model not effective loop couplings. In this model, loop-induced couplings are assumed to follow the SM structure as in arXiv:1209.0040. The best fit values of the parameters are shown, with the corresponding 68% and 95% CL intervals, and the overall p-value pSM of the SM Higgs hypothesis is given.
Summary of the fits for deviations in the coupling for the generic five-parameter model not effective loop couplings, expressed as function of the particle mass. For the fermions, the values of the fitted yukawa couplings hff are shown, while for vector bosons the square-root of the coupling for the hVV vertex divided by twice the vacuum expectation value of the Higgs boson field. Particle masses (in the MS-bar scheme) and the vacuum expectation value of the Higgs boson are taken from the PDG. In this model, loop-induced couplings are assumed to follow the SM structure as in arXiv:1209.0040.
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Summary of the fits for deviations in the coupling for the generic five-parameter model not effective loop couplings, expressed as function of the particle mass. For the fermions, the values of the fitted yukawa couplings hff are shown, while for vector bosons the square-root of the coupling for the hVV vertex divided by twice the vacuum expectation value of the Higgs boson field. Particle masses for leptons and weak boson, and the vacuum expectation value of the Higgs boson are taken from the PDG. For the top quark the same mass used in theoretical calculations is used (172.5 GeV) and for the bottom quark the running mass mb(mH=125.7 GeV)=2.763 GeV is used. In this model, loop-induced couplings are assumed to follow the SM structure as in arXiv:1209.0040.
 

Combined WW + ZZ results for spin 2

 
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