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Emergence of large densities in a chemotaxis system with signal-dependent motility

Abstract

In this paper, we focus on the emergence of large densities of a cell population in finite time in the following parabolic-elliptic Keller-Segel system with signal-dependent motility and a source term of logistic type uε t = Δ(e−vεuε) + ε(κuε − μuε2) , 0 =Δvε−vε+ uε. in a smooth bounded domain Ω⊆ℝ2 with homogenuous Neumann boundary conditions and parameters κ,μ>0 and ε∈(0,1). We will show that the solution uε can exceed any certain value M>0 before a time T(M)>0 under the condition that ε>0 is sufficiently small. To prove the result, we show convergence of classical solutions of the first system to classical solutions of the corresponding limit system as εsearrow 0 ut=Δ(e−vu), −Δv+v=u. The main challenge is to find suitable bounds for uε and vε, that are ε-independent, in Lebesgue and Hölder spaces, whereas for fixed ε>0 global existence and boundedness is known.

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BibTeX
@misc{hegenbart2026emergence,
  title = {{Emergence of large densities in a chemotaxis system with signal-dependent motility}},
  author = {Max Hegenbart},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.36934},
  eprint = {2610.36934},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.36934},
}
RIS
TY  - UNPB
TI  - Emergence of large densities in a chemotaxis system with signal-dependent motility
AU  - Max Hegenbart
PY  - 2026
DA  - 2026/10/27
PB  - arXiv
DO  - 10.48550/arxiv.2610.36934
UR  - https://arxiv.org/abs/2610.36934
AB  - In this paper, we focus on the emergence of large densities of a cell population in finite time in the following parabolic-elliptic Keller-Segel system with signal-dependent motility and a source term of logistic type u_ε t = Δ(e^−v_εu_ε) + ε(κu_ε − μu_ε^2) , 0 =Δv_ε−v_ε+ u_ε. in a smooth bounded domain Ω⊆ℝ^2 with homogenuous Neumann boundary conditions and parameters κ,μ>0 and ε∈(0,1). We will show that the solution u_ε can exceed any certain value M>0 before a time T(M)>0 under the condition that ε>0 is sufficiently small. To prove the result, we show convergence of classical solutions of the first system to classical solutions of the corresponding limit system as εsearrow 0 u_t=Δ(e^−vu), −Δv+v=u. The main challenge is to find suitable bounds for u_ε and v_ε, that are ε-independent, in Lebesgue and Hölder spaces, whereas for fixed ε>0 global existence and boundedness is known.
ER  -