A sufficient condition for absence of mass quantization in a chemotaxis system with local sensing

We analyze blowup solutions in infinite time of the Neumann boundary value problem for the fully parabolic chemotaxis system with local sensing:$\begin{array}{c}\{\begin{array}{c}{u}_t=\Delta \left(e^{-v}u\right)\mathrm{in}\Omega \times (0,\infty ),\\ v_t=\Delta v-v+u\mathrm{in}\Omega \times (0,\infty ),\end{array}\end{array}$where $\Omega$ is a ball in two-dimensional space and with nonnegative radially symmetric initial data. In the case of the Keller–Segel system which has similar mathematical structures to our system, it was shown that solutions blow up in finite time if and only if $L\log L$ for the first component $u$ diverges in finite time. On the other hand, focusing on the variational structure induced by the signal-dependent motility function $e^{-v}$, we show that the unboundedness of ${\int }_{\Omega }{e}^{v}dx$ for the second component $v$ gives rise to blowup solutions in infinite time under the assumption of radial symmetry. Moreover we prove mass concentration phenomena at the origin. It is shown that the radially symmetric solutions of our system develop a singularity like a Dirac delta function in infinite time. Here we investigate the weight of this singularity. Consequently it is shown that mass quantization may not occur; that is, the weight of the singularity can exceed $8\pi$ under the assumption of a uniform-in-time lower bound for a Lyapunov functional. This type of behavior cannot be observed in the Keller–Segel system.