  We investigate a general $U(1)_X$ scenario where we introduce three
generations of Standard Model (SM) singlet Right Handed Neutrinos (RHNs) to
generate the light neutrino mass through the seesaw mechanism after the
breaking of $U(1)_X$ and electroweak symmetries. In addition to that, a general
$U(1)_X$ scenario involves an SM-singlet scalar field and due to the $U(1)_X$
symmetry breaking the mass of a neutral beyond the SM (BSM) gauge boson
$Z^\prime$ is evolved. The RHNs, being charged under $U(1)_X$ scenario, can
explain the origin of observed baryon asymmetry through the resonant
leptogenesis process. Applying observed neutrino oscillation data we study
$Z^\prime$ and BSM scalar induced processes to reproduce the observed baryon
asymmetry. Hence we estimate bounds on the $U(1)_X$ gauge coupling $(g_X)$ and
the mass of the $Z^\prime$ $(M_{Z^\prime})$ for different $U(1)_X$ charges and
benchmark masses of RHN and SM-singlet scalar. Finally we compare our results
with limits obtained from the existing limits from LEP-II and LHC. We find that
depending on the $U(1)_X$ charges, the masses of RHNs and SM-singlet scalar
resonant leptogenesis could provide stronger limit on $g_X$ for $M_{Z^\prime} >
5.8$ TeV which could be probed by high energy scattering experiment in future.
