When can we uniquely map a classical density to a time-dependent potential?

Abstract

When can we uniquely map the dynamic evolution of a classical density to a time-dependent potential? In equilibrium, without time dependence, the one-body density uniquely specifies the external potential that is applied to the system. This mapping from a density to the potential is the cornerstone of classical density functional theory (DFT). In this talk, we derive rigorous and explicit conditions for such a unique mapping between a nonequilibrium density profile and a time-dependent external potential. We thus prove the underlying assertion of dynamical density functional theory (DDFT) - with or without the so-called adiabatic approximation often used in applications. We also illustrate loopholes when our conditions are violated so that two distinct external potentials result in the same density profiles but different currents, as suggested by the framework of power functional theory (PFT).