Encoding equilibrium states of matter in the format of phase diagrams is among the basic and at the same time most fruitful concepts in solid-state and materials chemistry. The appealing stringency of these concepts is related to the fact that any equilibrium state of matter, as characterized by its phase content (defined by the phases present, their compositions, and concentrations) and the respective activities of the components, is unambiguously determined by fixing the set of independent variables of state, p (or V), T, x iÀ1 for a system constituted of i components. In many fields of science and technology, analyzing chemical processes in terms of phase diagrams and equilibrium thermodynamics has proven an invaluable tool. [1][2][3] In spite of the impressive success of such an approach in specific areas, it fails seriously in addressing the full "real" materials world, since most of the matter around us stays trapped in metastable, in many cases quite persistent, states. Even at demanding thermal conditions, for example, prevailing in gas or steam turbines, many of the materials employed are not in equilibrium. Quite generally, it is easy to show that metastable materials are of substantial relevance: durable diamond is metastable at ambient conditions, glasses constitute an economically significant class of matter, and (metastable) amorphous ceramics can outperform thermodynamically stable crystalline ones with respect to the overall set of properties relevant for high-temperature applications. [4,5] As a consequence, a holistic consideration of a given chemical system, for example, for the purpose of synthesis planning, needs to include both the equilibrium and the metastable states. [6,7] Thus it would be highly desirable to address metastable states of matter in a similarly rational way as thermodynamically stable ones and to put both on a comparable footing. Regarding the most popular presentation of equilibrium phase diagrams that are obtained by projecting the lowest parts of the Gibbs energy surfaces of the competing thermodynamically stable phases onto the space spanned by the variables (p, T, x i ), such an objective would imply to perform an analogous procedure for metastable matter. After identifying all chemical compounds and phases that are capable of existence, one would determine their free energies as a function of the thermodynamic boundary conditions, and directly derive graphical representations (analogous to equilibrium phase diagrams) from this information. Noteworthy, such a procedure requires to involve the temperaturedependent lifetime of the metastable state under consideration as a further parameter.In the past, it has been shown that known features of equilibrium phase diagrams can be extra-and interpolated, as well as checked for consistency, by the well-known CAL-PHAD approach.[8] Furthermore, for a known configuration, its internal energy can be calculated, and, by considering the respective thermal excitations, the free energy can be derived,where G el and G magn refer to the...