The three-dimensional Anderson model with a rectangular distribution of sit
e disorder displays two distinct localization-delocalization transitions, a
gainst varying disorder intensity, for a relatively narrow range of Fermi e
nergies. Such transitions are studied through the calculation of Localizati
on lengths of quasi-one-dimensional systems by transfer-matrix methods, and
their analysis by finite-size scaling techniques. For the transition at hi
gher disorder we iind the localization-length exponent nu = 1.60(5) and the
limiting scaled localization-length amplitude Lambda (0) =0.57(1), strongl
y suggesting universality with the transition at the band center, for which
currently accepted values are nu =1.57(2) and Lambda (0) =0.576(2). For th
e lower (reentrant) transition, we estimate nu = 1.55(15) and Lambda (0) =0
.55(5), still compatible with universality but much less precise, partly ow
ing to significant finite-size corrections.