We explore the evolution of wave-function statistics on a finite Bethe lattice (Cayley tree) from the central site (“root”) to the boundary (“leaves”). We show that the eigenfunction moments $P_q=N \left<|\psi|^{2q}(i)\right>P_q\propto N^{-\tau_q}NN\to\infty$. The multifractality spectrum depends on the strength of disorder and on the parameter characterizing the position of the observation point on the lattice. Specifically, , where is the distance from the observation point to the root, and is the “radius” of the lattice. We demonstrate that the exponents depend linearly on and determine the evolution of the spectrum with increasing disorder, from delocalized to the localized phase. Analytical results are obtained for the -orbital model with that can be mapped onto a supersymmetric model. These results are supported by numerical simulations (exact diagonalization) of the conventional () Anderson tight-binding model.

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