  We show that the signature of two boosted $W$-jets plus large missing energy
is very promising to probe heavy charged resonances ($X^\pm$) through the
process of $pp\to X^+X^-\to W^+W^- X^0 X^0$ where $X^0$ denotes dark matter
candidate. The hadronic decay mode of the $W$ boson is considered to maximize
the number of signal events. When the mass split between $X^\pm$ and $X^0$ is
large, one has to utilize the jet-substructure technique to analyze the boosted
$W$-jet. For illustration we consider the process of chargino pair production
at the LHC, i.e., $pp\to \chi_1^+\chi^-_1 \to W^+W^-\chi_1^0\chi_1^0$, and
demonstrate that the proposed signature is able to cover more parameter space
of $m_{\chi_1^\pm}$ and $m_{\chi_1^0}$ than the conventional signature of
multiple leptons plus missing energy. More importantly, the signature of our
interests is not sensitive to the spin of heavy resonances.
