  The nuclear modification factors ($R_{AA}$) of $\pi^{\pm}, p(\bar p)$, and
$d(\bar d)$ with $|y|<0.5, p_T<20.0$~GeV/c in peripheral (40-60\%) and central
(0-5\%) Pb-Pb collisions at $\sqrt {s_{NN}}=2.76$ TeV have been studied using
the parton and hadron cascade ({\footnotesize PACIAE}) model plus the
dynamically constrained phase space coalescence ({\footnotesize DCPC}) model.
It is found that the $R_{AA}$ of light (anti)nuclei ($d, \bar d$) is similar to
that of hadrons ($\pi^\pm, p, \bar p$), and the $R_{AA}$ of antiparticles is
the same as that of particles. The suppression of $R_{AA}$ at high-$p_T$
strongly depends on event centrality and mass of the particles, i.e., the
central collision is more suppressed than the peripheral collision. Besides,
the yield ratios and double ratios for different particle species in $pp$ and
Pb-Pb collisions are discussed, respectively. It is observed that the yield
ratios and double ratios of $d$ to $p$ and $p$ to $\pi$ are similar to those of
their anti-particles in three different collision systems, suggesting that the
suppressions of matter ($\pi^{+}, p, d$) and the corresponding antimatter
($\pi^{-},\bar{p},\bar{d}$) are around the same level.
