Changes between Version 110 and Version 111 of ALRM

Timestamp:

Oct 13, 2016, 6:40:56 PM (8 years ago)

Author:

Mustafa Ashry

Comment:

--

ALRM

@@ -20 +20 @@
 
 
-
 As any other left-right symmetric model, ALRM is a QFT gauged by ''SU(3)_C×SU(2)_L×SU(2)_R×U(1)_B-L''. The latter ''B'' and ''L'' being the baryon and lepton numbers. An extra discrete symmetry ''S'' is imposed to distinguish between Higgs fields and their dual fields and hence their interactions.
 
@@ -33 +32 @@
 Minimization conditions and spectrum relations are all used to express the whole model parameters and spectra in terms of only five independent (external) parameters: ''tanbeta, lambda_2, lambda_3, alpha_1, alpha_2''. As in any two-Higgs doublet model, e.g., MSSM, ''tanbeta'' is the ratio between two vevs. The parameters ''lambda_2, lambda_3, alpha_1, alpha_2'' are dimensionless potential parameters. The charged Higgs masses are implemented as external parameters.
 
-The effective loop-induced h->gg and h->gammagamma, Zgamma, ZZ decays were added. For the complete pp->gammagamma analysis, Madgraph, Pythia and Madanalysis were used to produce this histogram figure (to be improved):[[Image(https://feynrules.irmp.ucl.ac.be/attachment/wiki/ALRM/pp-%3Egammagamma.png)]].
+The effective loop-induced h->gg and h->gammagamma, Zgamma, ZZ decays were added. For the complete pp->gammagamma analysis, '''''Madgraph''''', Pythia and Madanalysis were used to produce this histogram figure (to be improved):[[Image(https://feynrules.irmp.ucl.ac.be/attachment/wiki/ALRM/pp-%3Egammagamma.png)]].
 
 '''References'''