Absolutely continuous spectrum of the 3D Anderson model at weak disorder · revision history

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Title
Absolutely continuous spectrum of the 3D Anderson model at weak disorder
Plain
Prove that at least some electron states in a weakly disordered 3D lattice spread over the whole sample. This is the half of the mobility-edge problem that has no proof at all.
Precise
For $H = \Delta + \lambda V$ on $\ell^2(Z^3)$, with $\Delta$ the nearest-neighbour hopping operator (spectrum $[-6, 6]$ at $\lambda = 0$), i.i.d. bounded $V$ and $\lambda$ small, prove that the almost-sure spectrum has a nonzero absolutely continuous component in some energy interval inside $(-6, 6)$, or at least that eigenfunctions in that interval are not exponentially localized. Answer: a proof.
Settled by
A proof of absolutely continuous spectrum, or of delocalized eigenfunctions in finite volume uniformly in the volume, for $d = 3$.
Kind
well-posed
Answer type
proof
References
(empty)
Literature status
open
Status note
Absolutely continuous spectrum at weak disorder is proven on tree graphs (Klein, 1998, and later work of Aizenman and Warzel), not on $Z^d$.
Posed since
1958