Weakly pumped systems with approximate conservation laws can be
efficiently described by (generalized) Gibbs ensembles if the steady
state of the system is unique. However, such a description can fail if
there are multiple steady state solutions, for example, a bistability.
In this case domains and domain walls may form. In one-dimensional (1D)
systems any type of noise (thermal or non-thermal) will in general lead
to a proliferation of such domains. We study this physics in a 1D spin
chain with two approximate conservation laws, energy and the
zz-component
of the total magnetization. A bistability in the magnetization is
induced by the coupling to suitably chosen Lindblad operators. We
analyze the theory for a weak coupling strength
\epsilonϵ
to the non-equilibrium bath. In this limit, we argue that one can use
hydrodynamic approximations which describe the system locally in terms
of space- and time-dependent Lagrange parameters. Here noise terms
enforce the creation of domains, where the typical width of a domain
wall goes as \sim 1/\sqrt{\epsilon}∼1/ϵ
while the density of domain walls is exponentially small in
1/\sqrt{\epsilon}1/ϵ.
This is shown by numerical simulations of a simplified hydrodynamic
equation in the presence of noise.