  We report the investigation of the kinetic freeze-out properties of
identified hadrons ($\pi^\pm$, $K^\pm$ and $p(\bar p)$) along with light
(anti-)nuclei $d (\bar d)$, $t (\bar t)$ and ${}^{3}He$ in relativistic
heavy-ion collisions at RHIC and LHC energies. A simultaneous fit is performed
with the Blast-Wave (BW) model to the transverse momentum ({\ppt}) spectra of
identified hadrons together with light (anti-)nuclei produced in $Au+Au$
collisions at {\sqrtsNN} = 7.7 -- 200 GeV at the RHIC and in $Pb+Pb$ collisions
at $\sqrt{\mathrm{s}_{_{\mathrm{NN}}}}$ = 2.76 TeV at the LHC. The energy and
centrality dependence of freeze-out parameters, i.e., kinetic freeze-out
temperature ($T_{kin}$) and collective flow velocity $\langle \beta \rangle$
has been studied. It is observed that light (anti-)nuclei also participate in
the collective expansion of the medium created in the collision when included
in a common fit with the light hadrons. We observe a marginal rise in $T_{kin}$
and a slight decrease in $\langle \beta \rangle$ when compared to the values
obtained from the fit to light hadrons. A similar $\langle \beta \rangle$ and
significantly larger $T_{kin}$ is observed when a fit is performed to only
protons and light (anti-)nuclei. Both, $T_{kin}$ and $\langle \beta \rangle$
show a weak energy dependence at most collision energies.
