The long-standing problem of the Hall resistivity rho(xy) in the Hall insul
ator phase is addressed using four-lead Chalker-Coddington networks. Electr
on interaction effects are introduced via a finite dephasing length. In the
quantum coherent regime, we find that rho(xy) scales with the longitudinal
resistivity rho(xx), and they both diverge exponentially with the dephasin
g length. In the Ohmic limit (where the dephasing length is shorter than th
e Hall puddle size), rho(xy). remains quantized and independent of rho(xx).
This suggests a new experimental probe for dephasing processes. [S0031-900
7(99)08338-3].