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NMSSM

The Next-to-Minimal Supersymmetric Standard Model (NMSSM) is an extension of the MSSM that adds a gauge-singlet chiral superfield S. It is motivated by the μ problem of the MSSM, where the supersymmetric μ parameter must be near the electroweak scale but is otherwise arbitrary. In the NMSSM, μ is generated dynamically as μ_eff = λ ⟨S⟩, tying it to the vacuum expectation value of the singlet and the electroweak scale.

The model is defined by a superpotential that typically includes the MSSM matter terms with the MSSM

The Higgs sector of the NMSSM contains three CP-even and two CP-odd neutral Higgs bosons (in the

Phenomenologically, the λ term can raise the tree-level mass of the SM-like Higgs, helping address aspects of

μ-term
replaced
by
λ
S
H_u
H_d
plus
a
self-interaction
κ
S^3/3
in
the
Z3-symmetric
version.
After
S
acquires
a
vacuum
expectation
value,
an
effective
μ-term
is
generated.
The
NMSSM
expands
the
neutral
fermion
sector
with
a
singlino,
resulting
in
five
neutralinos,
and
enlarges
the
Higgs
sector.
CP-conserving
limit),
in
addition
to
the
charged
Higgses.
The
mixing
with
the
singlet
can
give
rise
to
lighter
singlet-dominated
states
and
altered
couplings.
Consequently,
new
decay
modes
may
appear,
such
as
a
SM-like
Higgs
decaying
into
lighter
pseudoscalars
or
other
Higgs
states.
the
hierarchy
problem.
The
NMSSM
provides
viable
dark
matter
candidates,
often
with
a
singlino
component,
and
offers
distinctive
collider
signatures
due
to
the
extended
Higgs
and
neutralino
sectors.
Variants
include
the
scale-invariant
NMSSM
and
models
with
explicit
μ
terms;
a
Z3
symmetry
can
introduce
a
domain-wall
problem,
typically
resolved
by
small
explicit
breaking
terms
or
higher-dimensional
operators.