  In this paper, we consider the dynamics of R\'enyi negativities after a
quantum quench in the free-boson chain with homogeneous dissipation. Initially
we prepare the system in the squeezed thermal state, and then let it evolves
under the tight-binding bosonic Hamiltonian with local linear dissipation. We
use the Lindblad equation to solve the time evolution of the covariance matrix,
from which one can obtain the time dependence of R\'enyi negativities. We are
interested in the weak dissipation hydrodynamic limit where a quasi-particle
picture emerges. In this limit, exact results of non-equilibrium dynamics of
R\'enyi negativities can be obtained using the stationary phase method. We
consider the R\'enyi negativities between both adjacent and disjoint regions in
a infinite chain. We numerically test our analytical predictions and perfect
matches have found.
