  The Imry-Ma phenomenon, predicted in 1975 by Imry and Ma and rigorously
established in 1989 by Aizenman and Wehr, states that first-order phase
transitions of low-dimensional spin systems are `rounded' by the addition of a
quenched random field to the quantity undergoing the transition. The phenomenon
applies to a wide class of spin systems in dimensions $d\le 2$ and to spin
systems possessing a continuous symmetry in dimensions $d\le 4$.
  This work provides quantitative estimates for the Imry--Ma phenomenon: In a
cubic domain of side length $L$, we study the effect of the boundary conditions
on the spatial and thermal average of the quantity coupled to the random field.
We show that the boundary effect diminishes at least as fast as an inverse
power of $\log\log L$ for general two-dimensional spin systems and for
four-dimensional spin systems with continuous symmetry, and at least as fast as
an inverse power of $L$ for two- and three-dimensional spin systems with
continuous symmetry. Specific models of interest for the obtained results
include the two-dimensional random-field $q$-state Potts and Edwards-Anderson
spin glass models, and the $d$-dimensional random-field spin $O(n)$ models
($n\ge 2$) in dimensions $d\le 4$.
