  This article deals with the study of the following Kirchhoff-Choquard
problem:
  \begin{equation*}
  \begin{array}{cc}
  \displaystyle M\left(\, \int\limits_{\mathbb{R}^N}|\nabla u|^p\right)
(-\Delta_p) u + V(x)|u|^{p-2}u = \left(\,
\int\limits_{\mathbb{R}^N}\frac{F(u)(y)}{|x-y|^{\mu}}\,dy \right) f(u),
\;\;\text{in} \; \mathbb{R}^N,
  u > 0, \;\; \text{in} \; \mathbb{R}^N,
  \end{array}
  \end{equation*}
  where $M$ models Kirchhoff-type nonlinear term of the form $M(t) = a +
bt^{\theta-1}$, where $a, b > 0$ are given constants; $1<p<N$, $\Delta_p =
\text{div}(|\nabla u|^{p-2}\nabla u)$ is the $p$-Laplacian operator; potential
$V \in C^2(\mathbb{R}^N)$; $f$ is monotonic function with suitable growth
conditions. We obtain the existence of a positive high energy solution for
$\theta \in \left[1, \frac{2N-\mu}{N-p}\right) $ via the Poho\v{z}aev manifold
and linking theorem. Apart from this, we also studied the radial symmetry of
solutions of the associated limit problem.
