Advances in High Energy Physics / 2012 / Article / Tab 1 / Research Article
Higgs Bosons Near 125 GeV in the NMSSM with Constraints at the GUT Scale Table 1 Properties of two benchmark points corresponding to different values of
𝑀
𝐻
1
. All dimensionful parameters are given in GeV. The components of
𝜒
0
1
, as well as the components of
𝐻
𝑖
, are defined such that their squares sum up to 1. The Susy contributions
Δ
𝑎
𝜇
to the muon anomalous magnetic moment are those given by NMSSMTools without any theoretical errors.
Point
(
1
)
(
2
)
Param. at
𝑀
G
U
T
:
𝑀
1
/
2
6
0
0
5
2
5
𝑚
0
6
0
0
9
6
0
𝐴
0
−
1
5
5
0
−
1
1
4
0
𝐴
𝜆
−
6
2
5
−
5
7
5
𝐴
𝜅
−
2
7
5
−
3
6
0
𝑚
𝐻
𝑢
1
6
7
0
1
8
8
0
𝑚
𝐻
𝑑
4
4
5
7
5
7
𝑚
𝑆
8
8
5
1
3
8
0
𝜆
0
.
9
6
1
.
4
8
𝜅
0
.
7
3
1
.
0
8
ℎ
𝑡
0
.
8
3
0
.
9
7
Param. at
𝑀
S
u
s
y
:
𝜆
0
.
5
4
5
0
.
6
𝜅
0
.
2
5
3
0
.
3
2
1
t
a
n
𝛽
2
.
4
0
2
.
2
9
𝜇
e
ff
1
2
0
1
2
2
Sparticle masses:
𝑚
̃
𝑔
1
3
9
0
1
2
5
0
𝑚
̃
𝑞
1
3
2
0
1
4
0
0
𝑚
̃
𝑡
1
3
5
9
4
6
3
𝑚
̃
𝑏
1
1
0
0
1
1
0
6
0
𝑚
̃
𝜏
1
5
2
8
9
0
0
𝑀
𝜒
±
1
1
0
8
1
0
8
𝑀
𝜒
0
1
7
7
7
8
Components of
𝜒
0
1
:
𝐵
0
.
2
0
0
.
2
5
𝑊
−
0
.
1
6
−
0
.
2
0
𝐻
𝑑
0
.
4
8
0
.
5
2
𝐻
𝑢
−
0
.
7
0
−
0
.
7
0
𝑆
0
.
4
6
0
.
3
7
Ω
ℎ
2
0
.
1
0
0
.
1
0
𝜎
𝑠
𝑖
(
𝑝
)
[
1
0
−
8
pb]
1
.
0
0
0
.
1
3
Δ
𝑎
𝜇
[
1
0
−
1
0
]
0
.
9
3
0
.
5
2
𝑀
𝐻
1
100 120 Components of
𝐻
1
:
𝐻
𝑑
0
.
3
9
0
.
5
0
𝐻
𝑢
0
.
3
4
0
.
7
4
𝑆
0
.
8
6
0
.
4
5
𝑅
1
𝛾
𝛾
(
𝑔
𝑔
)
0
.
0
1
0
.
3
2
𝑅
1
𝛾
𝛾
(
V
B
F
)
0
.
0
3
0
.
4
0
𝑅
1
𝑉
𝑉
(
𝑔
𝑔
)
0
.
0
3
0
.
3
4
𝑅
1
𝜏
𝜏
(
V
B
F
)
0
.
2
3
0
.
8
8
𝑀
𝐻
2
1
2
4
1
2
5
Components of
𝐻
2
:
𝐻
𝑑
0
.
2
6
0
.
0
4
𝐻
𝑢
0
.
8
5
−
0
.
5
4
𝑆
−
0
.
4
5
0
.
8
4
𝑅
2
𝛾
𝛾
(
𝑔
𝑔
)
1
.
5
4
1
.
7
7
𝑅
2
𝛾
𝛾
(
V
B
F
)
1
.
4
2
0
.
9
8
𝑅
2
𝑉
𝑉
(
𝑔
𝑔
)
1
.
2
2
1
.
0
1
𝑅
2
𝜏
𝜏
(
V
B
F
)
0
.
6
3
0
.
0
3
𝑀
𝐻
3
3
2
9
3
0
5
Components of
𝐻
3
:
𝐻
𝑑
0
.
8
8
0
.
8
6
𝐻
𝑢
−
0
.
4
0
−
0
.
4
0
𝑆
−
0
.
2
5
−
0
.
3
0
𝑅
3
𝛾
𝛾
(
𝑔
𝑔
)
0
.
2
1
0
.
2
9
𝑅
3
𝛾
𝛾
(
V
B
F
)
0
.
0
0
0
6
0
.
0
0
0
7
𝑅
3
𝑉
𝑉
(
𝑔
𝑔
)
0
.
0
0
1
0
.
0
0
2
𝑅
3
𝜏
𝜏
(
V
B
F
)
0
.
0
4
0
.
0
3