  Two opposite charged new heavy gauge boson pair production at the Large
Hadron Collider (LHC) is presented in this paper. These bosons are known as
$W^{'}$ boson due to the reason that it is the heavy version of Standard
Model's weak force carrier, the $W$ boson. The production cross section and
decay width in proton-proton ($pp$) collision at \sqrts~= 8 TeV are calculated
for different masses and coupling strengths of $W^{'}$. Efficiencies for
different signal regions and branching ratios for different decay channels are
computed. In this study, the pair production ($W^{'^{+}}W^{'^{-}}$) is
considered in emerging new physics as a result of $pp$ collision at \sqrts~= 8
TeV at the LHC with final state containing two tau ($\tau$) leptons and two
neutrinos (each $W^{'}$ decay to $\tau$ and its neutrino). The event selection
efficiency similar to the CMS experiment is used for the mass of $W^{'}$ to set
lower limits for different coupling strengths of $W^{'}$ and results are
presented in this work. For heavy gauge bosons, when coupling strength is
similar to that of Standard Model's $W$ boson, the mass of $W^{'}$ below 305
GeV are excluded at confidence level of $95\%$.
