Let be a positive harmonic function in the unit ball $B_1 \subset ^n\muux\in \partial B_1n(x)x\alpha(-1,n-1]A \in [0,+\infty) u(x+n(x)t)t^{\alpha} \to At \to +0\frac{\mu({B_r(x)})}{r^{n-1}} r^{\alpha} \to C_\alpha Ar\to+0{C_\alpha= \frac{\pi^{n/2}}{\Gamma(\frac{n-\alpha+1}{2})\Gamma(\frac{\alpha+1}{2})}}\alpha=0$ it follows from the theorems by Rudin and Loomis which claim that a positive harmonic function has a limit along the normal iff the boundary measure has the derivative at the corresponding point of the boundary. For it concerns about the point mass of at and it follows from the Beurling minimal principle. For the general case of $\alpha \in (-1,n-1)$ we prove it with the help of the Wiener Tauberian theorem in a similar way to Rudin’s approach. Unfortunately this approach works for a ball or a half-space only but not for a general kind of domain. In dimension one can use conformal mappings and generalise the statement above to sufficiently smooth domains, in dimension we showed that this generalisation is possible for due to harmonic measure estimates. The last method leads to an extension of the theorems by Loomis, Ramey and Ullrich on non-tangential limits of harmonic functions to positive solutions of elliptic differential equations with Holder continuous coefficients.

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