  We obtain the entanglement negativity for various bipartite zero and finite
temperature pure and mixed state configurations in a class of
$(1+1)$-dimensional Galilean conformal field theories. In this context we
establish a construction for computing the entanglement negativity for such
bipartite states involving a suitable replica technique. Our construction
exactly reproduces certain universal features observed for entanglement
negativity of corresponding states in relativistic $(1+1)$-dimensional
conformal field theories.
