Suppose we have a second order elliptic differential operator $$ L(v) = -\text{div}(A(x) \nabla v) $$ $A(x)$ is a bounded and strictly positive definite matrix with Hölder continuous entries. And suppose $\Omega$ is a $C^1$ domain (can be considered more regular if required). From [2, Theorem 1], we know that there exists a Poisson Kernel $K(x,y)$ for the above operator and domain $\Omega$. That is the solution $u$ such that $Lu=0$ in $\Omega$ can be written as $$ u(x) = \int_{\partial \Omega}u(y) K(x,y) d\mathcal H^{N-1}(y) $$ On the other hand, we have from [1] we have the existence of Green's function $G$ for the operator $L$ in the domain $\Omega$. Natural question to ask is just like we have a integral representation for harmonic functions, can we say that the Poisson Kernel $K(x,y)$ and the co-normal derivative of Green's function on the boundary i.e. $\left ( A(y)\nabla_y G(x,y)\right )\cdot \nu $ are equal on $\partial \Omega$? In particular, since the Green's function $G$ of $L$ exists for the domain $\Omega$, then for $u$ such that $Lu=0$ is the following expression true? $$ u(x) = \int_{\partial \Omega}u(y) \left ( A(y)\nabla_y G(x,y)\right )\cdot \nu\,d\mathcal H^{N-1}(y). $$ The above claim hods true when $A(x)= Id$, i.e. when the operator $L$ is simple Laplacian. Under what condition/s we can say the same for a general second order elliptic operator in divergence form? [1] <cite authors="Grueter, Michael; Widman, Kjell-Ove">_Grueter, Michael; Widman, Kjell-Ove_, [**The Green function for uniformly elliptic equations**](http://dx.doi.org/10.1007/BF01166225), Manuscr. Math. 37, 303-342 (1982). [ZBL0485.35031](https://zbmath.org/?q=an:0485.35031).</cite> [2] <cite authors="Fabes, Eugene B.; Jerison, David S.; Kenig, Carlos E.">_Fabes, Eugene B.; Jerison, David S.; Kenig, Carlos E._, [**Necessary and sufficient conditions for absolute continuity of elliptic- harmonic measure**](http://dx.doi.org/10.2307/2006966), Ann. Math. (2) 119, 121-141 (1984). [ZBL0551.35024](https://zbmath.org/?q=an:0551.35024).</cite>