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The behavior of the two-particle spectral function, S (q, ), is examined in the hydrodynamic regime, at the mobility edge in a model for the integer quantized Hall effect. Results are presented from numerical diagonalization of the Hamiltonian for finite systems. For q^{2} small, S (q, ) has a conventional, diffusive form. For q^{2} large, the novel dependence S (q, ) ^-{2}q^-2+ is obtained, with =0. 380. 04.
Chalker et al. (Mon,) studied this question.