Abstract
This paper is concerned with the Keller--Segel system with flux limitation, \begin{align} \tag{$\ast$} \begin{cases} u_t=Δu - \nabla \cdot (uf(|\nabla v|^{2})\nabla v), \\ v_t=Δv - v + u \end{cases} \end{align} in bounded $n$-dimensional domains with homogeneous Neumann boundary conditions, where $f$ generalizes the prototype obtained on letting \[ f(ξ) = k_f(1 + ξ)^{-α}, \quad ξ\ge 0, \] with $k_f > 0$ and $α> 0$. In this framework, it is shown that if either $n = 1$ and $α> 0$ is arbitrary, or $n \ge 2$ and $α> \frac{n-2}{2(n-1)}$, then for any nonnegative initial data belonging to the space of Radon measures for the population density and to $W^{1,q}$ with $q \in (\max\{1, (1-2α)n\}, \frac{n}{n-1})$ for the signal density, there exists a global classical solution of the Neumann problem for $(\ast)$, which is continuous at $t = 0$ in an appropriate sense.

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