  Quantum systems are invariably open, evolving under surrounding influences
rather than in isolation. Standard open quantum system methods eliminate all
information on the environmental state to yield a tractable description of the
system dynamics. By incorporating a collective coordinate of the environment
into the system Hamiltonian, we circumvent this limitation. Our theory provides
straightforward access to important environmental properties that would
otherwise be obscured, allowing us to quantify the evolving system-environment
correlations. As a direct result, we show that the generation of robust
system-environment correlations that persist into equilibrium (heralded also by
the emergence of non-Gaussian environmental states) renders the canonical
system steady-state almost always incorrect. The resulting equilibrium states
deviate markedly from those predicted by standard perturbative techniques and
are instead fully characterised by thermal states of the mapped
system-collective coordinate Hamiltonian. We outline how noncanonical system
states could be investigated experimentally to study deviations from canonical
thermodynamics, with direct relevance to molecular and solid-state nanosystems.
