Abstract

Going beyond this, the present work focuses on the possible extent of unboundedness phenomena also on short timescales, and hence investigates in more detail the set of times in $(0,\infty)$ at which solutions may develop singularities. The main results in this direction reveal the existence of a global weak energy solution which coincides with a smooth function throughout $\overline{\Omega}\times E$, where $E$ denotes a countable union of open intervals which is such that $|(0,\infty)\setminus E|=0$. In particular, this indicates that a similar feature of the unperturbed Navier--Stokes equations, known as Leray’s structure theorem, persists even in the presence of the coupling to the attractive and hence potentially destabilizing cross-diffusive mechanism in the full system ($\star$).

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