  In this paper, based on the thin-shell formalism, we introduce a classical
model for particles in the framework of $n+1-$dimensional
$\left[\frac{n}{2}\right]$-order pure Lovelock gravity. In particular, we
construct a spherically symmetric particle of radius $a$ whose inside is a flat
Minkowski spacetime while its outside is charged pLG solution. Knowing that in
$n+1-$dimensional spherically symmetric Einstein gravity ($R$-gravity) such a
particle model cannot be constructed, as we have discussed first, provides the
main motivation for this study. In fact, it is the richness of Lovelock
parameters that provides such a particle construction possible. On the
thin-shell, the energy-momentum components are chosen to vanish, yet their
normal derivatives are non-zero.
