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On the stability of Type I self-similar blowups for the Keller-Segel system in three dimensions and higher
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abstract
We consider the parabolic-elliptic Keller-Segel system in spatial dimensions $d\geq3$, which corresponds to the mass supercritical case. Some solutions become singular in finite time, an important example being backward self-similar solutions. Herrero et al. and Brenner et al. showed the existence of such profiles, countably many in dimensions $3\leq d \leq 9$ and at least two for $d\geq 10$. We establish that all these self-similar profiles are stable along a set of initial data with finite Lipschitz codimension equal to the number of instable eigenmodes. This extends the recent finding of Glogi\'c et al. showing the stability of the fundamental self-similar profile. We obtain additional results, such as the possibility of the solutions we construct to originate from smooth and compactly supported initial data, their convergence at blow-up time, and the Lipschitz regularity of the blow-up time. Our proof extends the approach proposed in Collot et al., based on renormalizing the solution around a modulated self-similar solution, and using a spectral gap for the linearized operator in the parabolic neighbourhood of the singularity.
Forward citations
Cited by 3 Pith papers
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Nonradial stability of self-similar blowup to Keller-Segel equation in three dimensions
Any sufficiently small H^2 nonradial perturbation of the explicit 3D Keller-Segel self-similar blowup profile still blows up along the same self-similar profile with decaying error.
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Finite time blow-up for an inhomogeneous parabolic equation
For large n, a codimension-n Lipschitz manifold of nonradial data produces finite-time blow-up to the homogeneous self-similar profile Φ_n for the inhomogeneous heat equation in R^3 with p>5.
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Finite-time blow-up for the three dimensional axially symmetric Keller-Segel system
For any finite set of points in the half-plane of axial symmetry, there exists a 3D Keller-Segel solution whose mass concentrates at those points with a precisely quantified finite-time blow-up rate.
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