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Tobias Black

Publications and source records attributed to Tobias Black.

At least 19 recordsLinked to original sources

Avoidance of caldera-type dead cores in a chemotaxis system with degenerate diffusion and compactly supported initial population density

We consider a degenerate chemotaxis system of the form \begin{align}\label{star}\tag{$\star$} \left\lbrace \begin{array}{r@{}l@{\quad}l} &u_t=\nabla\cdot\big(D(u)\nabla u-uS(u)\nabla v\big)+f(u,v),\\ &v_t=Δv+g(u,v),\end{array}\right. \end{align} in a bounded domain $Ω\subset\mathbb{R}^{N}$ with smooth boundary subjected to no-flux and homogeneous Neumann boundary conditions. Herein, the diffusion coefficient $D\in C^0([0,\infty))\cap C^1((0,\infty))$ is assumed to satisfy $D(0)=0$ and $D'(s)\geq 0$ on $(0,\infty)$, and there are $s_0\in(0,1]$ and $d>0$ such that $D(s)\geq ds^{m-1}$ on $[0,s_0]$ and that \begin{align*} s D'(s)\leq C_D D(s)\quad\text{for }s\in[0,s_0]. \end{align*} The sensitivity function $S\in C^2([0,\infty))$ and the source term $f\in C^{1}([0,\infty)\times[0,\infty))$ in the first equation are supposed to be nonnegative. The source term $g\in C^{1}([0,\infty)\times[0,\infty))$ of the second equation can in fact be negative. Prototypical choices for $g$ are $g(u,v)=-uv$ and $g(u,v)=-v+u$. We show under suitable assumptions on weak solutions to \eqref{star} on $Ω\times(0,T_0)$, that whenever the smoothly bounded domain $ω\subset\mathbb{R}^N$ and $T\in(0,T_0)$ are such that \begin{align*} \overlineω\subseteq Ω,\qquad u_0>0\ \text{ in }\ \overlineω,\qquad\text{ and }\qquad u>0\ \text{ on }\ \partialω\times(0,T), \end{align*} then \begin{align*} u>0\quad\text{in }\ \overlineω\times[0,T). \end{align*} In particular, any dead cores that appear during the evolution must have developed from regions that were already part of the initial zero set.

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Subcritical-mass global solvability in a doubly degenerate Keller-Segel system with signal production

We consider the initial-boundary value problem for a variant of the Keller-Segel chemotaxis system with doubly degenerate diffusion, i.e. we study \[ \left\{ \begin{array}{ll} u_t = \nabla \cdot (uv\nabla u) - \nabla \cdot (u^2v\nabla v),\\ v_t = Δv + u - v,\\ (uv\nabla u-u^2v\nabla v)\cdotν=\nabla v\cdotν=0,\\ u(x,0)=u_0(x),\quad v(x,0)=v_0(x), \end{array} \right. \] in a smoothly bounded domain $Ω\subset\mathbb{R}^2$. Crucially, we only assume the sufficiently regular initial data to be nonnegative, but allow those functions to be zero at non-trivial parts of the domain. We show that, despite possibly starting from a degenerate state, the system admits global solutions in a framework of generalized energy solutions, whenever the initial mass is below the threshold number $m_0=4π$. Moreover, in a radial setting the threshold number can be increased to $m_0=8π$.

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Global solutions and large time stabilization in a model for thermoacoustics in a standard linear solid

This manuscript is concerned with the one-dimensional system \[ \begin{array}{l} τu_{ttt} + αu_{tt} = b \big(γ(Θ) u_{xt}\big)_x + \big( γ(Θ) u_x\big)_x, \\[1mm] Θ_t = D Θ_{xx} + bγ(Θ) u_{xt}^2, \end{array} \] which is connected to the simplified modeling of heat generation in Zener type materials subject to stress from acoustic waves. Under the assumption that the coefficients $τ>0, b>0$ and $α\geq0$ satisfy \begin{align}\tag{$\star$} αb >τ, \end{align} it is shown that for all $Θ_\star>0$ one can find $ν=ν(D,τ,α,b,Θ_\star,γ)>0$ such that an associated Neumann type initial-boundary value problem with Neumann data admits a unique time-global solution in a suitable framework of strong solvability whenever the initial temperature distribution fulfills $$\|Θ_0\|_{L^\infty(Ω)}\leq Θ_\star$$ and the derivatives of the initial data are sufficiently small in the sense of satisfying $$\int_Ωu_{0xx}^2 + \int_Ω(u_{0t})_{xx}^2 + \int_Ω(u_{0tt})_x^2 < ν\quad\text{and}\quad \|Θ_{0x}\|_{L^\infty(Ω)} + \|Θ_{0xx}\|_{L^\infty(Ω)} < ν.$$ The constructed solution moreover features an exponential stabilization property for both components. In particular, the parameter range described by ($\star$) coincides with the full stability regime known for the corresponding Moore--Gibson--Thompson equation despite the fairly strong nonlinear coupling to the temperature variable.

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Refining Hölder regularity theory in degenerate drift-diffusion equations

We establish the Hölder continuity of bounded nonnegative weak solutions to \begin{align*} \big(Φ^{-1}(w)\big)_t=Δw+\nabla\cdot\big(a(x,t)Φ^{-1}(w)\big)+b\big(x,t,Φ^{-1}(w)\big), \end{align*} with convex $Φ\in C^0([0,\infty))\cap C^2((0,\infty))$ satisfying $Φ(0)=0$, $Φ'>0$ on $(0,\infty)$ and $$sΦ''(s)\leq CΦ'(s)\quad\text{for all }s\in[0,s_0]$$ for some $C>0$ and $s_0\in(0,1]$. The functions $a$ and $b$ are only assumed to satisfy integrability conditions of the form \begin{align*} a&\in L^{2q_1}\big((0,T);L^{2q_2}(Ω;\mathbb{R}^N)\big),\\ b&\in M\big(Ω_T\times\mathbb{R}\big)\ \text{such that }\big|b(x,t,ξ)\big|\leq \hat{b}(x,t)\ \text{a.e. for some }\hat{b}\in L^{q_1}\big((0,T);L^{q_2}(Ω)\big) \end{align*} with $q_1,q_2>1$ such that $$\frac{2}{q_1}+\frac{N}{q_2}=2-Nκ\quad\text{for some }κ\in(0,\tfrac{2}{N}).$$ Letting $w=Φ(u)$ and assuming the inverse $Φ^{-1}:[0,\infty)\to[0,\infty)$ to be locally Hölder continuous, this entails Hölder regularity for bounded weak solutions of $$u_t=ΔΦ(u)+\nabla\cdot\big(a(x,t)u\big)+b(x,t,u)$$ and, accordingly, covers a wide array of taxis type structures. In particular, many chemotaxis frameworks with nonlinear diffusion, which cannot be covered by the standard literature, fall into this category. After rigorously treating local Hölder regularity, we also extend the regularity result to the associated initial-boundary value problem for boundary conditions of flux-type.

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Very mild diffusion enhancement and singular sensitivity: Existence of bounded weak solutions in a two-dimensional chemotaxis-Navier--Stokes system

We consider an initial-boundary value problem for the chemotaxis-Navier--Stokes system \begin{align*} \left\{ \begin{array}{c@{\quad}l@{\quad}l@{\,}c} n_{t}+u\cdot\nabla n=\nabla\cdot\big(D(n)\nabla n-nS(x,n,c)\cdot\nabla c\big),\ &x\inΩ,& t>0,\\ c_{t}+u\cdot\nabla c=Δc-cn,\ &x\inΩ,& t>0,\\ u_{t}+(u\cdot\nabla)u=Δu+\nabla P+n\nablaΦ,\quad \nabla\cdot u=0,\ &x\inΩ,& t>0,\\ \big(D(n)\nabla n-nS(x,n,c)\cdot\nabla c)\cdotν=\nabla c\cdotν=0,\ u=0,\ &x\in\partialΩ,& t>0,\\ n(\cdot,0)=n_0,\ c(\cdot,0)=c_0,\ u(\cdot,0)=u_0,\ &x\inΩ. \end{array}\right. \end{align*} in a smoothly bounded domain $Ω\subset\mathbb{R}^2$. Assuming $S:\overlineΩ\times[0,\infty)\times(0,\infty)\rightarrow \mathbb{R}^{2\times 2}$ to be sufficiently regular and such that with $γ\in[0,\frac56]$ and some non-decreasing $S_0:(0,\infty)\to(0,\infty)$, we have \begin{align*} \big|S(x,n,c)\big|\leq \frac{S_0(c)}{c^γ}\quad\text{for all }(x,n,c)\in\overlineΩ\times[0,\infty)\times(0,\infty), \end{align*} we show that if $D:[0,\infty)\to[0,\infty)$ is suitably regular and positive throughout $(0,\infty)$, then for all $M>0$ one can find $L(M)>0$ such that whenever $$\liminf_{n\to\infty} D(n)>L\quad\text{and}\quad \liminf_{n\searrow0}\frac{D(n)}{n}>0$$ are satisfied and the initial data $(n_0,c_0,u_0)$ are suitably regular and satisfy $\|c_0\|_{L^{\infty}(Ω)}\leq M$ there is a global and bounded weak solution for the initial-boundary value problem above. Under the additional assumption of $D(0)>0$ this solution is moreover a classical solution of the same problem.

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Absence of dead-core formations in chemotaxis systems with degenerate diffusion

In this paper we consider a chemotaxis system with signal consumption and degenerate diffusion of the form \begin{align*} \left\lbrace \begin{array}{r@{}l@{\quad}l} &u_t=\nabla\cdot\big(D(u)\nabla u-uS(u)\nabla v\big)+f(u,v),\\ &v_t=Δv- uv,\\ \end{array}\right. \end{align*} in a bounded domain $Ω\subset\mathbb{R}^{N}$ with smooth boundary subjected to no-flux and homogeneous Neumann boundary conditions. Herein, the diffusion coefficient $D\in C^0([0,\infty))\cap C^2((0,\infty))$ is assumed to satisfy $D(0)=0$, $D(s)>0$ on $(0,\infty)$, $D'(s)\geq 0$ on $(0,\infty)$ and that there are $s_0>0$, $p>1$ and $C_D>0$ such that $$s D'(s)\leq C_D D(s)\quad\text{and}\quad C_D s^{p-1}\leq D(s)\quad\text{for }s\in[0,s_0].$$ The sensitivity function $S\in C^2([0,\infty))$ and the source term $f\in C^{1}([0,\infty)\times[0,\infty))$ are supposed to be nonnegative. We show that for all suitably regular initial data $(u_0,v_0)$ satisfying $u_0\geq δ_0>0$ and $v_0\not\equiv 0$ there is a time-local classical solution and - despite the degeneracy at $0$ - the solution satisfies an extensibility criterion of the form $$\text{either}\quad T_{max}=\infty,\quad\text{or}\quad\limsup_{t\nearrow T_{max}}\|u(\cdot,t)\|_{L^\infty(Ω)}=\infty.$$ Moreover, as a by-product of our analysis, we prove that a classical solution on $Ω\times(0,T)$ obeying $\|u(\cdot,t)\|_{L^\infty(Ω)}\leq M_u$ for all $t\in(0,T)$ and emanating from initial data $(u_0,v_0)$ as specified above remains strictly positive throughout $Ω\times(0,T)$, i.e. one can find $δ_u=δ_u(T,δ_0, M_u,\|v_0\|_{W^{1,\infty}(Ω)})>0$ such that $$u(x,t)\geqδ_u\quad\text{for all }(x,t)\inΩ\times(0,T).$$ Together, the results indicate that the formation of a dead-core in these chemotaxis systems with a degenerate diffusion are impossible before the blow-up time.

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Possible points of blow-up in chemotaxis systems with spatially heterogeneous logistic source

We discuss the influence of possible spatial inhomogeneities in the coefficients of logistic source terms in parabolic-elliptic chemotaxis-growth systems of the form \begin{align*} u_t &= Δu - \nabla\cdot(u\nabla v) + κ(x)u-μ(x)u^2, 0 &= Δv - v + u \end{align*} in smoothly bounded domains $Ω\subset\mathbb{R}^2$. Assuming that the coefficient functions satisfy $κ,μ\in C^0(\overlineΩ)$ with $μ\geq0$ we prove that finite-time blow-up of the classical solution can only occur in points where $μ$ is zero, i.e.\ that the blow-up set $\mathcal{B}$ is contained in \begin{align*} \big\{x\in\overlineΩ\midμ(x)=0\big\}. \end{align*} Moreover, we show that whenever $μ(x_0)>0$ for some $x_0\in\overlineΩ$, then one can find an open neighbourhood $U$ of $x_0$ in $\overlineΩ$ such that $u$ remains bounded in $U$ throughout evolution.

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Relaxed parameter conditions for chemotactic collapse in logistic-type parabolic-elliptic Keller-Segel systems

We study the finite-time blow-up in two variants of the parabolic-elliptic Keller-Segel system with nonlinear diffusion and logistic source. In $n$-dimensional balls, we consider \begin{align*} \begin{cases} u_t = \nabla \cdot ((u+1)^{m-1}\nabla u - u\nabla v) + λu - μu^{1+κ}, \\ 0 = Δv - \frac1{|Ω|} \int_Ωu + u \end{cases} \tag{JL} \end{align*} and \begin{align*} \begin{cases} u_t = \nabla \cdot ((u+1)^{m-1}\nabla u - u\nabla v) + λu - μu^{1+κ}, \\ 0 = Δv - v + u, \end{cases}\tag{PE} \end{align*} where $λ$ and $μ$ are given spatially radial nonnegative functions and $m, κ> 0$ are given parameters subject to further conditions. In a unified treatment, we establish a bridge between previously employed methods on blow-up detection and relatively new results on pointwise upper estimates of solutions in both of the systems above and then, making use of this newly found connection, provide extended parameter ranges for $m,κ$ leading to the existence of finite-time blow-up solutions in space dimensions three and above. In particular, for constant $λ, μ> 0$, we find that there are initial data which lead to blow-up in (JL) if \begin{alignat*}{2} 0 \leq κ&< \min\left\{\frac{1}{2}, \frac{n - 2}{n} - (m-1)_+ \right\}&&\qquad\text{if } m\in\left[\frac{2}{n},\frac{2n-2}{n}\right)\\ \text{ or }\quad 0 \leq κ&<\min\left\{\frac{1}{2},\frac{n-1}n-\frac{m}2\right\} &&\qquad \text{if } m\in\left(0,\frac{2}{n}\right), \end{alignat*} and in (PE) if $m \in [1, \frac{2n-2}{n})$ and \begin{align*} 0 \leq κ< \min\left\{\frac{(m-1) n + 1}{2(n-1)}, \frac{n - 2 - (m-1) n}{n(n-1)} \right\}. \end{align*}

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Prescribed signal concentration on the boundary: Weak solvability in a chemotaxis-Stokes system with proliferation

We study a chemotaxis-Stokes system with signal consumption and logistic source terms of the form \noindent \begin{align*} \left\{ \begin{array}{r@{\ }l@{\quad}l@{\quad}l@{\,}c} n_{t}+u\cdot\!\nabla n&=Δn-\nabla\!\cdot(n\nabla c)+κn-μn^{2},\ &x\inΩ,& t>0,\\ c_{t}+u\cdot\!\nabla c&=Δc-nc,\ &x\inΩ,& t>0,\\ u_{t}&=Δu+\nabla P+n\nablaϕ,\ &x\inΩ,& t>0,\\ \nabla\cdot u&=0,\ &x\inΩ,& t>0,\\ \big(\nabla n-n\nabla c\big)\cdotν&=0,\quad c=c_{\star}(x),\quad u=0, &x\in\partialΩ,& t>0, \end{array}\right. \end{align*} where $κ\geq0$, $μ>0$ and, in contrast to the commonly investigated variants of chemotaxis-fluid systems, the signal concentration on the boundary of the domain $Ω\subset\mathbb{R}^N$ with $N\in\{2,3\}$, is a prescribed time-independent nonnegative function $c_{\star}\in C^{2}\!\big(\overlineΩ\big)$. Making use of the boundedness information entailed by the quadratic decay term of the first equation, we will show that the system above has at least one global weak solution for any suitably regular triplet of initial data.

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Global generalized solutions to a forager-exploiter model with superlinear degradation and their eventual regularity properties

In this article we consider a cascaded taxis model for two proliferating and degrading species which thrive on the same nutrient but orient their movement according to different schemes. In particular, we assume the first group, the foragers, to orient their movement directly along an increasing gradient of the food density, while the second group, the exploiters, instead track higher densities of the forager group. Specifically, we will investigate an initial boundary-value problem for a prototypical forager-exploiter model of the form \begin{align*} \left\{ \begin{array}{r@{\,}c@{\,}l@{\quad }l@{\quad}l@{\quad}l@{\,}c} u_{t}&=&Δu-\nabla\cdot\big(u\nabla w\big)+f(u),\ &x\inΩ,& t>0,\\ v_{t}&=&Δv-\nabla\cdot\big(v\nabla u\big)+g(v),\ &x\inΩ,& t>0,\\ w_{t}&=&Δw-(u+v)w-μw+r(x,t),\ &x\inΩ,& t>0, \end{array}\right. \end{align*}%} in a smoothly bounded domain $Ω\subset\mathbb{R}^2$, where $μ\geq 0$, $r\in\ C^1(\barΩ\times[0,\infty))\cap L^\infty\!\left(Ω\times(0,\infty)\right)$ is nonnegative and the functions $f,g\in C^1\!\left([0,\infty)\right)$ are assumed to satisfy $f(0)\geq0$, $g(0)\geq0$ as well as $$-k_f s^α -l_f\leq f(s)\leq -K_f s^α+L_f\ \text{ and }\ -k_g s^β-l_g\leq g(s)\leq -K_g s^β+L_g\quad\text{for }s\geq0,$$ respectively, with constants $α,β>1$, $k_f,K_f,k_g,K_g>0$ and $l_f,L_f,l_g,L_g\geq0$ and $α,β>1$. Assuming that $α>1+\sqrt{2}$, $\min\{α,β\}>\frac{α+1}{α-1}$ and that $r$ satisfies certain structural conditions we establish the global solvability of this system with respect to a suitable generalized solution concept and then, for the more restrictive case of $α,β>1+\sqrt{2}$ and $μ>0$, investigate an eventual regularity effect driven by the decay of the nutrient density $w$.

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The Stokes limit in a three-dimensional chemotaxis-Navier-Stokes system

We consider initial-boundary value problems for the $κ$-dependent family of chemotaxis-(Navier--)Stokes systems \begin{align*} \left\{ \begin{array}{r@{\,}c@{\,}c@{\ }l@{\quad}l@{\quad}l@{\,}c} n_{t}&+&u\cdot\!\nabla n&=Δn-\nabla\!\cdot(n\nabla c),\ &x\inΩ,& t>0,\\ c_{t}&+&u\cdot\!\nabla c&=Δc-cn,\ &x\inΩ,& t>0,\\ u_{t}&+&κ(u\cdot\nabla)u&=Δu+\nabla P+n\nablaϕ,\ &x\inΩ,& t>0,\\ &&\nabla\cdot u&=0,\ &x\inΩ,& t>0, \end{array}\right. \end{align*} in a bounded domain $Ω\subset\mathbb{R}^3$ with smooth boundary and given potential function $ϕ\in C^{1+β}(\overlineΩ)$ for some $β>0$. It is known that for fixed $κ\in\mathbb{R}$ an associated initial-boundary value problem possesses at least one global weak solution $(n^{(κ)},c^{(κ)},u^{(κ)})$, which after some waiting time becomes a classical solution of the system. In this work we will show that upon letting $κ\to0$ the solutions $(n^{(κ)},c^{(κ)},u^{(κ)})$ converge towards a weak solution of the Stokes variant $(κ=0)$ of the systems above with respect to the strong topology in certain Lebesgue and Sobolev spaces. We thereby extend the recently obtained result on the Stokes limit process for classical solutions in the two-dimensional setting to the more intricate three-dimensional case.

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Stabilization in the Keller--Segel system with signal-dependent sensitivity

This paper deals with the Keller--Segel system with signal-dependent sensitivity \begin{align*} &u_t = Δu - χ\nabla \cdot (uS(v)\nabla v), &v_t = Δv - v + u, \end{align*} where $χ>0$ and $S$ is a given function generalizing the sensitivity $S(s)=\frac{1}{(a+s)^{k}}$, $k>1$, $a\ge 0$, and shows exponential convergence of global classical solutions under an additional smallness condition condition for $χ>0$.

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Global solvability of chemotaxis-fluid systems with nonlinear diffusion and matrix-valued sensitivities in three dimensions

In this work we extend a recent result to chemotaxis fluid systems which include matrix-valued sensitivity functions $S(x,n,c):Ω\times[0,\infty)^2\to\mathbb{R}^{3\times3}$ in addition to the porous medium type diffusion, which were discussed in the previous work. Namely, we will consider the system \begin{align*} \left\{ \begin{array}{r@{\,}c@{\,}c@{\ }l@{\quad}l@{\quad}l@{\,}c} n_{t}&+&u\cdot\!\nabla n&=Δn^m-\nabla\!\cdot(nS(x,n,c)\nabla c),\ &x\inΩ,& t>0,\\ c_{t}&+&u\cdot\!\nabla c&=Δc-c+n,\ &x\inΩ,& t>0,\\ u_{t}&+&(u\cdot\nabla)u&=Δu+\nabla P+n\nablaϕ,\ &x\inΩ,& t>0,\\ &&\nabla\cdot u&=0,\ &x\inΩ,& t>0, \end{array}\right. \end{align*} in a bounded domain $Ω\subset\mathbb{R}^3$ with smooth boundary. Assuming that $m\geq1$, $α\geq0$ satisfy $m+α>\frac43$, that the matrix-valued function $S(x,n,c):Ω\times[0,\infty)^2\to\mathbb{R}^{3\times3}$ satisfies $|S(x,n,c)|\leq\frac{S_0}{(1+n)^α}$ for some $S_0>0$ and suitably regular nonnegative initial data, we show that the corresponding no-flux-Dirichlet boundary value problem emits at least one global very weak solution. Upon comparison with results for the fluid-free system this condition appears to be optimal. Moreover, imposing a stronger condition for the exponents $m$ and $α$, i.e. $m+2α>\frac{5}{3}$, we will establish the existence of at least one global weak solution in the standard sense.

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Global very weak solutions to a chemotaxis-fluid system with nonlinear diffusion

We consider the chemotaxis-fluid system \begin{align}\label{star}\tag{$\diamondsuit$} \left\{ \begin{array}{r@{\,}c@{\,}c@{\ }l@{\quad}l@{\quad}l@{\,}c} n_{t}&+&u\cdot\!\nabla n&=Δn^m-\nabla\!\cdot(n\nabla c),\ &x\inΩ,& t>0,\\ c_{t}&+&u\cdot\!\nabla c&=Δc-c+n,\ &x\inΩ,& t>0,\\ u_{t}&+&(u\cdot\nabla)u&=Δu+\nabla P+n\nablaϕ,\ &x\inΩ,& t>0,\\ &&\nabla\cdot u&=0,\ &x\inΩ,& t>0, \end{array}\right. \end{align} in a bounded domain $Ω\subset\mathbb{R}^3$ with smooth boundary and $m>1$. Assuming $m>\frac{4}{3}$ and sufficiently regular nonnegative initial data, we ensure the existence of global solutions to the no-flux-Dirichlet boundary value problem for \eqref{star} under a suitable notion of very weak solvability, which in different variations has been utilized in the literature before. Comparing this with known results for the fluid-free setting of \eqref{star} the condition appears to be optimal with respect to global existence. In case of the stronger assumption $m>\frac{5}{3}$ we moreover establish the existence of at least one global weak solution in the standard sense. In our analysis we investigate a functional of the form $\int_Ω\! n^{m-1}+\int_Ω\! c^2$ to obtain a spatio-temporal $L^2$ estimate on $\nabla n^{m-1}$, which will be the starting point in deriving a series of compactness properties for a suitably regularized version of \eqref{star}. As the regularity information obtainable from these compactness results vary depending on the size of $m$, we will find that taking $m>\frac{5}{3}$ will yield sufficient regularity to pass to the limit in the integrals appearing in the weak formulation, while for $m>\frac{4}{3}$ we have to rely on milder regularity requirements making only very weak solutions attainable.

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A Keller-Segel-fluid system with singular sensitivity: Generalized solutions

In bounded smooth domains $Ω\subset\mathbb{R}^N$, $N\in\{2,3\}$, we consider the Keller-Segel-Stokes system \begin{align*} n_t + u\cdot \nabla n &= Δn - χ\nabla \cdot(\frac{n}{c}\nabla c),\\ c_t + u\cdot \nabla c &= Δc - c + n,\\ u_t &= Δu + \nabla P + n\nabla ϕ, \qquad \nabla \cdot u=0, \end{align*} and prove global existence of generalized solutions if \[ χ<\begin{cases} \infty,&N=2,\\ \frac{5}{3},&N=3. \end{cases} \] These solutions are such that blow-up into a persistent Dirac-type singularity is excluded.

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Singular sensitivity in a Keller-Segel-fluid system

In bounded smooth domains $Ω\subset\mathbb{R}^N$, $N\in\{2,3\}$, considering the chemotaxis--fluid system \[ \begin{cases} \begin{split} & n_t + u\cdot \nabla n &= Δn - χ\nabla \cdot(\frac{n}{c}\nabla c) &\\ & c_t + u\cdot \nabla c &= Δc - c + n &\\ & u_t + κ(u\cdot \nabla) u &= Δu + \nabla P + n\nabla Φ& \end{split}\end{cases} \] with singular sensitivity, we prove global existence of classical solutions for given $Φ\in C^2(\barΩ)$, for $κ=0$ (Stokes-fluid) if $N=3$ and $κ\in\{0,1\}$ (Stokes- or Navier--Stokes fluid) if $N=2$ and under the condition that \[ 0<χ<\sqrt{\frac{2}{N}}. \]

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Global generalized solutions to a parabolic-elliptic Keller-Segel system with singular sensitivity

We investigate the parabolic-elliptic Keller-Segel model \begin{align*}\left\{\begin{array}{r@{\,}l@{\quad}l@{\quad}l@{\,}c} u_{t}&=Δu-\,χ\nabla\!\cdot(\frac{u}{v}\nabla v),\ &x\inΩ,& t>0,\\ 0&=Δv-\,v+u,\ &x\inΩ,& t>0,\\ \frac{\partial u}{\partialν}&=\frac{\partial v}{\partialν}=0,\ &x\in\partialΩ,& t>0,\\ u(&x,0)=u_0(x),\ &x\inΩ,& \end{array}\right. \end{align*} in a bounded domain $Ω\subset\mathbb{R}^n$ $(n\geq2)$ with smooth boundary. \noindent We introduce a notion of generalized solvability which is consistent with the classical solution concept, and we show that whenever $0<χ<\frac{n}{n-2}$ and the initial data satisfy only certain requirements on regularity and on positivity, one can find at least one global generalized solution.

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Eventual smoothness of generalized solutions to a singular chemotaxis-Stokes system

We study the chemotaxis-fluid system \begin{align*} \left\{ \begin{array}{r@{\,}c@{\,}c@{\ }l@{\quad}l@{\quad}l@{\,}c} n_{t}&+&u\cdot\!\nabla n&=Δn-\nabla\!\cdot(\frac{n}{c}\nabla c),\ &x\inΩ,& t>0, c_{t}&+&u\cdot\!\nabla c&=Δc-nc,\ &x\inΩ,& t>0, u_{t}&+&\nabla P&=Δu+n\nablaϕ,\ &x\inΩ,& t>0, &&\nabla\cdot u&=0,\ &x\inΩ,& t>0, \end{array}\right. \end{align*} under homogeneous Neumann boundary conditions for $n$ and $c$ and homogeneous Dirichlet boundary conditions for $u$, where $Ω\subset\mathbb{R}^2$ is a bounded domain with smooth boundary and $ϕ\in C^{2}\left(\barΩ\right)$. From recent results it is known that for suitable regular initial data, the corresponding initial-boundary value problem possesses a global generalized solution. We will show that for small initial mass $\int_Ω\!n_0$ these generalized solutions will eventually become classical solutions of the system and obey certain asymptotic properties. Moreover, from the analysis of certain energy-type inequalities arising during the investigation of the eventual regularity, we will also derive a result on global existence of classical solutions under assumption of certain smallness conditions on the size of $n_0$ in $L^1\!\left(Ω\right)$ and in $L\log L\!\left(Ω\right)$, $u_0$ in $L^4\!\left(Ω\right)$, and of $\nabla c_0$ in $L^2\!\left(Ω\right)$.

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