"Fluid polyamorphism" is the existence of different condensed amorphous
states in a single-component fluid. It is either found or predicted, usually at
extreme conditions, for a broad group of very different substances, including
helium, carbon, silicon, phosphorous, sulfur,tellurium, cerium, hydrogen and
tin tetraiodide. This phenomenon is also hypothesized for metastable and deeply
supercooled water, presumably located a few degrees below the experimental
limit of homogeneous ice formation. We present a generic phenomenological
approach to describe polyamorphism in a single-component fluid, which is
completely independent of the molecular origin of the phenomenon. We show that
fluid polyamorphism may occur either in the presence or the absence of fluid
phase separation depending on the symmetry of the order parameter. In the
latter case, it is associated with a second-order transition, such as in liquid
helium or liquid sulfur. To specify the phenomenology, we consider a fluid with
thermodynamic equilibrium between two distinct interconvertible states or
molecular structures. A fundamental signature of this concept is the
identification of the equilibrium fraction of molecules involved in each of
these alternative states. However, the existence of the alternative structures
may result in polyamorphic fluid phase separation only if mixing of these
structures is not ideal. The two-state thermodynamics unifies all the debated
scenarios of fluid polyamorphism in different areas of condensed-matter
physics, with or without phase separation, and even goes beyond the phenomenon
of polyamorphism by generically describing the anomalous properties of fluids
exhibiting interconversion of alternative molecular states.Comment: 56 pages, including 39 pages of main text with 7 figures and 117
references, and 17 pages of supplemental material with 12 figures and 19
reference