Infinite-temperature thermostats by energy localization in a nonequilibrium setup

Some lattice models having two conservation laws may display an equilibrium phase transition from a homogeneous (positive temperature - PT) to a condensed (negative temperature) phase, where a finite fraction of the energy is localized in a few sites. We study one such stochastic model in an out-of-equilibrium setup, where the ends of the lattice chain are attached to two PT baths. We show that localized peaks may spontaneously emerge, acting as infinite-temperature heat baths. The number $N_b$ of peaks is expected to grow in time $t$ as $N_b \sim \sqrt{\ln t}$, as a consequence of an effective freezing of the dynamics. Asymptotically, the chain spontaneously subdivides into three intervals: the two external ones lying inside the PT region; the middle one characterized by peaks superposed to a background lying along the infinite-temperature line. In the thermodynamic limit, the Onsager formalism allows determining the shape of the whole profile.