  We provide a simple solution to the $\mu/B_\mu$ problem in the gauge-mediated
Next-to-Minimal Supersymmetric Standard Model. In this model the messenger
sector contains one pair of $3+\bar 3$ and one pair of $2+\bar 2$ messengers.
These two messenger pairs couple to different gauge singlets in the hidden
sector in which supersymmetry (SUSY) is broken. Such a gauge-mediation
structure can naturally arise in many backgrounds. Because of the two effective
SUSY breaking scales $\frac{< F_i>}{< M_i>}$ in the messenger sector, the
renormalization group evolutions of the soft SUSY breaking parameters can be
properly modified, leading to a negative enough singlet soft mass square
$m_N^2(\Lambda_{EW})$ and hence reasonable $\mu/B_\mu$ values. In most of the
perturbative (up to the GUT scale) parameter region, as a result, the
electroweak scale is stabilized and phenomenologically interesting mass spectra
of particles and superparticles are obtained. In addition, this model favors
large values of $\tan\beta$: $5 \sim 50$ and a heavy scalar spectrum. With the
relatively large $\tan\beta$, the light $U(1)_R$ pseudoscalar (mainly appearing
in the low-scale gauge-mediated SUSY breaking models) becomes extremely
singlet-like, and is no longer a problem in this model. These features apply to
all cases of low-, intermediate- and high-scale gauge-mediated SUSY breaking.
