In this manuscript, we investigate a boundary value problem governed by a complex system of partial differential equations given by: \(\begin{aligned} \displaystyle -\text{ div }\Big [{{\mathcal {L}}}_\vartheta \left( z,\vartheta ,\nabla \vartheta \right) \Big ]+{\hat{M}}\vert \vartheta \vert ^{p-2} \vartheta ={\mathcal {L}}_\sigma \Big (z, \hbar *\sigma (\vartheta ), \nabla (\hbar *\sigma (\vartheta ))\Big ), \end{aligned}\) under the following non-homogeneous Neumann boundary condition: \({\mathcal {L}}_\vartheta \left( z,\vartheta ,\nabla \vartheta \right) .\nu =\Theta (z,\vartheta )\) . Here, the functions \({\mathcal {L}}_\vartheta \) , \({\mathcal {L}}_\sigma \) , and \(\Theta \) exhibit Carathéodory characteristics. The operator \(\sigma : W^{1, p}({\mathcal {B}}) \rightarrow W^{1, p}\left( {\mathbb {R}}^N\right) \) operates as an extension operator correlated with the domain \({\mathcal {B}}\) , while \(\hbar \) denotes an integrable function defined over \({\mathbb {R}}^N\) . Notably, the problem introduces a nonlocal operator, manifesting as the convolution \(\hbar *\sigma (\vartheta )\) of \(\hbar \) with \(\sigma (\vartheta )\) , associated with the variable \(\vartheta \) . Under conditions necessitating thorough examination, we establish the existence of a weak solution to the mentioned problem by employing the topological degree method.