Changes between Version 3 and Version 4 of TwoHiggsDoublet

Timestamp:

Apr 13, 2012, 5:48:40 PM (13 years ago)

Author:

Olivier Mattelaer

Comment:

--

TwoHiggsDoublet

@@ -6 +6 @@
 more than twenty years, even though it has often been only
 considered as the scalar sector of larger models like the MSSM
-\citeGunion:1989we} or Little Higgs models
+\cite{Gunion:1989we} or Little Higgs models
 \cite{Arkani-Hamed:2002qx}. The generic 2HDM considered here may
 display by itself an interesting phenomenology justifying its
@@ -69 +69 @@
 The scalar potential in the Higgs basis reads 
 
-%$
-V &=& \mu_1 H_1^\dag H_1 +\mu_2 H_2^\dag H_2-\left(\mu_3 H_1^\dag H_2+\mathrm{h.c.}\right)\\
-  & & \lambda_1 \left(H_1^\dag H_1\right)^2+ \lambda_2 \left(H_2^\dag
-  H_2\right)^2\\ & & + \lambda_3 \left(H_1^\dag
-  H_1\right)\left(H_2^\dag H_2\right)+ \lambda_4 \left(H_1^\dag
-  H_2\right)\left(H_2^\dag H_1\right)\\ & & +\left[\left( \lambda_5
-  H_1^\dag H_2 + \lambda_6 H_1^\dag H_1+ \lambda_7 H_2^\dag
-  H_2\right)\left(H_1^\dag H_2\right)+\mathrm{h.c.}\right]\,.
-$%
+$V = \mu_1 H_1^\dag H_1 +\mu_2 H_2^\dag H_2-\left(\mu_3 H_1^\dag H_2+\mathrm{h.c.}\right) \lambda_1 \left(H_1^\dag H_1\right)^2+ \lambda_2 \left(H_2^\dagH_2\right)^2  + \lambda_3 \left(H_1^\dag H_1\right)\left(H_2^\dag H_2\right)+ \lambda_4 \left(H_1^\dag H_2\right)\left(H_2^\dag H_1\right) +\left[\left( \lambda_5 H_1^\dag H_2 + \lambda_6 H_1^\dag H_1+ \lambda_7 H_2^\dag H_2\right)\left(H_1^\dag H_2\right)+\mathrm{h.c.}\right]\,. $
 
 All parameters in front of quartic terms and the charged Higgs mass
@@ -90 +82 @@
 In the same basis, the Yukawa interactions read
 
-%$
-\mathcal{L}''Y&=&\frac{\overline{Q''L}\sqrt{2}}{v}\left[(M_d H_1 +   Y_d   H_2)d_R+(M_u \tilde{H}''1 +   Y''u   \tilde{H}''2)u''R\right]\\
-& &+\frac{\overline{E_L}\sqrt{2}}{v}\left[(M_e H_1 +   Y_e   H_2)e_R\right]\,.
-$%
+$\mathcal{L}''=Y\frac{\overline{Q''L}\sqrt{2}}{v}\left[(M_d H_1 +   Y_d   H_2)d_R+(M_u \tilde{H}''1 +   Y''u   \tilde{H}''2)u''R\right] +\frac{\overline{E_L}\sqrt{2}}{v}\left[(M_e H_1 +   Y_e   H_2)e_R\right]\,.$
 
 Yukawa couplings are expected to be given in the physical basis for