It has long been believed that equilibrium random-field Ising model (RFIM) critical scattering studies are not feasible in dilute antiferromagnets close to and below Tc(H) because of severe non-equilibrium effects. The high magnetic concentration Ising antiferromagnet F e0.93Zn0.07F2, however, does provide equilibrium behavior. We have employed scaling techniques to extract the universal equilibrium scattering line shape, critical exponents ν = 0.87 ± 0.07 and η = 0.20 ± 0.05, and amplitude ratios of this RFIM system.Models for the statistical physics of phase transitions can be experimentally tested by measuring the universal critical parameters and comparing them with theoretical predictions. This is crucial for the understanding of difficult problems such as the random-field Ising model (RFIM). Although it is well known that a phase transition occurs [1] for the d = 3 RFIM, the characterization of the equilibrium critical behavior in its experimental realization, anisotropic randomly dilute antiferromagnets such as F e x Zn 1−x F 2 in applied uniform fields [2], has not been possible near to and below the transition, T c (H), despite years of intense experimental investigation. This is primarily a result of the severe hysteresis in the scattering line shapes near to and below T c (H). Although long-range order is observed after cooling in zero field (ZFC) and heating through the transition, upon cooling through the transition in the field (FC) long-range antiferromagnetic order is never achieved, even at low temperatures. In either case, the line shapes are difficult to interpret. It was widely thought for many years that these nonequilibrium effects were unavoidable.Since random-field effects increase with the dilution, as well as the strength of the applied magnetic field [3], most early studies focused on magnetic concentrations x < 0.8 in order to achieve, for reasonable H, a suitable range of reduced temperature, t = (T − T c (H))/T c (H), over which asymptotic critical behavior might be observed. However, nonequilibrium effects exist below the equilibrium temperature [4] T eq (H) which lies just above T c (H). Much effort was directed to understanding the behavior of the domains, both near to and below T c (H). Neutron scattering studies of the Bragg intensity in the bulk crystal [5] F e 0.46 Zn 0.54 F 2 and the epitaxial film [6] of F e 0.52 Zn 0.48 F 2 showed anomalous behavior even under ZFC caused by domain formation. It was shown that, at low T , RFIM dynamics are dominated by domains [7,8]. The dominance of domain effects near T c (H) was evident in ac susceptibility measurements [9]. From these studies over several years along with Monte-Carlo (MC) simulations [10,11] it became clear that the severe nonequilibrium effects were primarily due to the large number of vacancies that are well connected and thus allow the formation of domain walls with insignificant energy cost.Recently, we demonstrated [12] that the metastability problem can, in fact, be overcome by employing a magnetically concentrate...