1 Correction to: J Comput Electron (2018) 17:427–435 https://doi.org/10.1007/s10825-017-1073-9

The original version of this article unfortunately contained a typographical error, and it has been corrected with this erratum. The first sub-section “Posing of the boundary value problem” intends to proceed with the introduction of the following integro-differential operators \({\varvec{R}}\) and \({\varvec{D}}\)

$$\varvec{R}\left( {\xi \left( q \right)} \right) = \int\limits_{{{\Gamma }}} {\xi \left( p \right)\frac{{\partial {\mathcal{G}}_{2} \left( {q,p} \right)}}{{\partial n^{\prime}}}dl^{\prime } } ,$$
$$\varvec{D}\left( {\xi \left( q \right)} \right) = \int\limits_{{{\Gamma }}} {\xi \left( p \right)\frac{{\partial ^{2} {\mathcal{G}}_{2} \left( {q,p} \right)}}{{\partial n\partial n^{\prime}}}dl^{\prime } }$$

in addition to the correctly presented \({\varvec{S}}\) and \({\varvec{V}}\).