An N-level quantum system is coupled to a bosonic heat reservoir at
positive temperature. We analyze the system-reservoir dynamics in the following
regime: The strength λ of the system-reservoir coupling is fixed and
small, but larger than the spacing σ of system energy levels. For
vanishing σ there is a manifold of invariant system-reservoir states and
for σ>0 the only invariant state is the joint equilibrium. The manifold
is invariant for σ=0 but becomes quasi-invariant for σ>0. Namely,
on a first time-scale of the order 1/λ2, initial states approach the
manifold. Then they converge to the joint equilibrium state on a much larger
time-scale of the order λ2/σ2. We give a detailed expansion of
the system-reservoir evolution showing the above scenario.Comment: Annales Henri Poincare 201