- #1
Safinaz
- 259
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Homework Statement
Hi,
I study the Higss sector of the MSSM from this review " arxiv:0503173v2", "The Higgs bosons in the Minimal Supersymmetric Model",
In Sec.: 1.2, it gives the Higgs potential by Equ. (1.60), then after acquiring the vevs and minimizing the potential to get the masses of the Higgs bosons , it yields two minimization conditions (1.70)
Homework Equations
I can not get Equ. (1.70)
The Attempt at a Solution
First I wrote the potential of the neutral components of the Higgs doublets: ## H_1,~ H_2##, as following:
$$ V_{H^0} = \bar{m}^2_1 |H^0_1|^2 + \bar{m}^2_2 |H^0_2|^2 + 2 B \mu H^0_1 H^0_2 + \frac{g_1^2+ g_2^2}{8} ( |H^0_1|^2 - |H^0_2|^2)^2.$$
Then minimized the potential
$$ \frac{\partial v }{\partial H_1^0} = \bar{m}^2_1 H^0_1 + 2 B \mu H^0_2 + \frac{g_1^2+ g_2^2}{4} ( |H^0_1|^2 - |H^0_2|^2) H^0_1=0, $$
$$ \frac{\partial v }{\partial H_2^0} = \bar{m}^2_2 H^0_2 + 2 B \mu H^0_1 -\frac{g_1^2+ g_2^2}{4} ( |H^0_1|^2 - |H^0_2|^2) H^0_2=0, $$
taking the minima Equ. (1.67), and using Equ. (1.68) and (1.61) in the reference, I got,
$$ ( \mu^2 +m_{H_1}^2) v_1 + 2 B \mu v_2 + \frac{M_z^2}{v^2} ( v_1^2 - v_2^2) v_1=0, $$
$$ ( \mu^2 +m_{H_2}^2) v_2 + 2 B \mu v_1 - \frac{M_z^2}{v^2} ( v_1^2 - v_2^2) v_2=0, $$
But then what I do to reach (1.70) ?
Thanks