  When a system consists of a large subsystem (bath) and a small one (probe),
thermalization implies induction of temperature of the bath onto the probe. If
both the bath and the probe are described by same microscopic Hamiltonian,
thermalization further entails that the probe imbibes the phase of the bath. We
refer to this phenomenon as phase thermalization. However, it is not clear
whether this phenomenon is realizable when the probe and the bath are described
by different microscopic Hamiltonians. We show phase thermalization is possible
even when the microscopic Hamiltonians differ significantly. We provide an
explicit example, where the probe is a Fermi liquid realized by a Majorana
chain with $n \gg 1$ fermions per site interacting through random hopping and
the bath is an incoherent metal described by another Majorana chain with $N >
n$ fermions per site interacting through arbitrarily long range random
four-fermion interaction. In deep infrared, the probe turns into an incoherent
metal, with Lyapunov spectrum and diffusion coefficient identical to the bath.
