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Jiashan Zheng

Publications and source records attributed to Jiashan Zheng.

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Global solvability in a higher-dimensional chemotaxis system for Alopecia Areata: Nonlinear proliferation versus logistic degradation

This paper is concerned with the Neumann initial-boundary value problem for the chemotaxis system: $u_t=Δu-χ_1\nabla\cdot(u\nabla w)+w-μ_1u^{r_1}$, $v_t=Δv-χ_2\nabla\cdot(v\nabla w)+w+ruv-μ_2v^{r_2}$, and $w_t=Δw+u+v-w$ in $Ω\times(0,\infty)$, which was initially proposed by Dobreva et al. to describe the dynamics of hair loss in Alopecia Areata form. Here, $Ω\subset\mathbb R^{N}$ $(N\geq3)$ is a smooth bounded domain, and the parameters fulfill $χ_{i}>0$, $μ_{i}>0$, $r_{i}\geq2$ $(i=1,2)$ and $r>0$. The inherent presence of two positive chemotaxis terms, along with the zero-order nonlinear production term $ruv$, significantly complicates the energy estimation. It is proved that if $r_{1}=r_{2}=2$ and $\min\{μ_{1},μ_{2}\}>μ^{\star}$ or $r_{i}>2$ $(i=1,2)$, this problem admits a global bounded classical solution for all sufficiently smooth initial data. The lower bound is given by $μ^{\star}=\frac{2(N-2)_{+}}{N}C_{\frac{N}{2}+1}^{\frac{1}{\frac{N}{2}+1}}\max\{χ_{1},χ_{2}\}+\left[(\frac{2}{N})^{\frac{2}{N+2}}\frac{N}{N+2}\right]r$, where $C_{\frac{N}{2}+1}$ is a positive constant corresponding to the maximal Sobolev regularity. Furthermore, we demonstrate that the basic assumption $μ_{i}>0$ $(i=1,2)$ is sufficient to guarantee the global existence of weak solutions for $N\geq3$. Notably, our findings not only extend or refine several existing results (see Remarks 1.1-1.2) but also provide new insights into the weak solution theory of this system for the first time.

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Some further progress for existence and boundedness of solutions to a two-dimensional chemotaxis-(Navier-)Stokes system modeling coral fertilization

In this paper, we investigate the effects exerted by the interplay among Laplacian diffusion, chemotaxis cross diffusion and the fluid dynamic mechanism on global existence and boundedness of the solutions. The mathematical model considered herein appears as \begin{align}\left\{ \begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot( nS(n)\nabla c)-nm,\quad x\in Ω, t>0, \disp{ c_{ t}+u\cdot\nabla c=Δc-c+w},\quad x\in Ω, t>0, \disp{w_{t}+u\cdot\nabla w=Δw-nw},\quad x\in Ω, t>0,\\ u_t+κ(u \cdot \nabla)u+\nabla P=Δu+(n+m)\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0,\quad x\in Ω, t>0,\\ \end{array}\right.\eqno(KSNF) \end{align} in a bounded domain $Ω\subset \mathbb{R}^2$ with a smooth boundary, which describes the process of coral fertilization occurring in ocean flow. Here $κ\in \mathbb{R}$ is a given constant, $ϕ\in W^{2,\infty}(Ω)$and $S(n) $ is a scalar function satisfies $|S(n)|\leq C_S(1+n)^{-α}$ {for all} $n\geq 0$ with some $C_S>0$ and $α\in\mathbb{R}$. It is proved that if either $α>-1,κ=0$ or $α\geq-\frac{1}{2},κ\in\mathbb{R}$ is satisfied,then for any reasonably smooth initial data, the corresponding Neumann-Neumann-Neumann-Dirichlet initial-boundary problem $(KSNF)$ possesses a globally classical solution. In case of the stronger assumption $α>-1,κ= 0$ or $α>-\frac{1}{2},κ\in\mathbb{R},$ we moreover show that the corresponding initial-boundary problem admits a unique global classical solution which is uniformly bounded on $Ω\times(0,\infty)$.

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Wellposedness of solution for an $N$-D chemotaxis-convection model during tumor angiogenesis

In this paper, we consider the following parabolic-parabolic-elliptic system } \begin{align*} \left\{\aligned & u_t=Δu-\nabla\cdot(u\nabla v)+ξ\nabla\cdot(u\nabla w)+au-μu^α, && x\inΩ, t>0,\\ & v_t=Δv+\nabla\cdot(v\nabla w)-v+u,&& x\inΩ, t>0,\\ & 0=Δw-w+u,&& x\inΩ, t>0\\ \endaligned\right. \end{align*} on a bounded domain $Ω\subset \mathbb{R}^{N}$ ($N\geq1$) with smooth boundary $\partial Ω$, where $μ$, $a$, $α$ are positive constants and $ξ\in\mathbb{R}$. If one of the following cases holds:\\ (i) $N\geq4$ and $α>\frac{4N-4+N\sqrt{2N^2-6N+8}}{2N}$;\\ (ii) $N=3$, $α>2$, for any $μ>0$ or $α=2$, the index $μ$ should be suitably big;\\ (iii) $N=2$, $α\geq2$, for any $μ>0$.\\ Without any restriction on the index $ξ$, for any given suitably regular initial data, the corresponding Neumann initial-boundary problem admits a unique global and bounded classical solution.

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A new result for boundedness of solutions to a quasilinear higher-dimensional chemotaxis -- haptotaxis model with nonlinear diffusion

This paper deals with a boundary-value problem for a coupled quasilinear chemotaxis--haptotaxis model with nonlinear diffusion $$\left\{\begin{array}{ll} u_t=\nabla\cdot(D(u)\nabla u)-χ\nabla\cdot(u\nabla v)-ξ\nabla\cdot(u\nabla w)+μu(1-u-w),\\ v_t=Δv- v +u,\quad \\ w_t=- vw\\ \end{array}\right. $$ in $N$-dimensional smoothly bounded domains, where the parameters $ξ,χ> 0$, $μ> 0$. The diffusivity $D(u)$ is assumed to satisfy $D(u)\geq C_{D}u^{m-1}$ for all $u > 0$ with some $C_D>0$. Relying on a new energy inequality, in this paper, it is proved that under the conditions $$m>\frac{2N}{N+{{{\frac{(\frac{\max_{s\geq1}λ_0^{\frac{1}{{s}+1}} (χ+ξ\|w_0\|_{L^\infty(Ω)})}{(\max_{s\geq1}λ_0^{\frac{1}{{s}+1}}(χ+ξ\|w_0\|_{L^\infty(Ω)})-μ)_{+}}+1) (N+\frac{\max_{s\geq1}λ_0^{\frac{1}{{s}+1}}(χ+ξ\|w_0\|_{L^\infty(Ω)})}{(\max_{s\geq1}λ_0^{\frac{1}{{s}+1}} (χ+ξ\|w_0\|_{L^\infty(Ω)})-μ)_{+}}-1)}{N}}}}},$$ and proper regularity hypotheses on the initial data, the corresponding initial-boundary problem possesses at least one global bounded classical solution when $D(0) > 0$ (the case of non-degenerate diffusion), while if, $D(0)\geq 0$ (the case of possibly degenerate diffusion), the existence of bounded weak solutions for system is shown. This extends some recent results by several authors.

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Global boundedness of the fully parabolic Keller-Segel system with signal-dependent motilities

This paper establishes the global uniform-in-time boundedness of solutions to the following Keller-Setel system with signal-dependent diffusion and chemotaxis \begin{equation}\left\{ \begin{array}{ll} u_t=\nabla\cdot(γ(v)\nabla u - uϕ(v)\nabla v),\quad & x\in Ω, t>0,\\ v_t = dΔv- v+u,\quad & x\in Ω, t>0 \end{array}\right.\end{equation} in a bounded domain $Ω\subset\mathbb{R}^N(N\leq4)$ with smooth boundary, where the density-dependent motility functions $γ(v)$ and $ϕ(v)$ denote the diffusive and chemotactic coefficients, respectively. The model was originally proposed by Keller and Segel in \cite{Keller-1} to describe the aggregation phase of Dictyostelium discoideum cells, where the two motility functions satisfy a proportional relation $χ(v)=(α-1)γ'(v)$ with $α>0$ denoting the ratio of effective body length (i.e. distance between receptors) to the step size. The major technical difficulty in the analysis is the possible degeneracy of diffusion. In this work, we show that if $γ(v)>0$ and $ϕ(v)>0$ are smooth on $[0,\infty)$ and satisfy $$\inf_{v\geq0} \frac{dγ(v)}{vϕ(v)(vϕ(v)+d-γ(v))_+}>\frac{N}{2},$$ then the above Keller-Segel system subject to Neumann boundary conditions admits classical solutions uniformly bounded in time. The main idea of proving our results is the estimates of a weighted functional $\int_Ωu^{p}v^{-q}dx$ for $p>\frac{N}{2}$ by choosing a suitable exponent $p$ depending on the unknown $v$, by which we are able to derive a uniform $L^\infty$-norm of $v$ and hence rule out the diffusion degeneracy.

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Boundedness and large time behavior in a higher-dimensional Keller--Segel system with singular sensitivity and logistic source

This paper focuses on the following Keller-Segel system with singular sensitivity and logistic source $$ \left\{\begin{array}{ll} u_t=Δu-χ\nabla\cdot(\frac{u}{v}\nabla v)+ au-μu^2,\quad x\in Ω, t>0, \disp{ v_t=Δv- v+u},\quad x\in Ω, t>0 \end{array}\right.\eqno(\star) $$ in a smoothly bounded domain $Ω\subset\mathbb{R}^N(N\geq1)$, with zero-flux boundary conditions, where $a>0,μ>0$ and $χ>0$ are given constants. If $χ$ is small enough, then, for all reasonable regular initial data, a corresponding initial-boundary value problem for $(\star)$ possesses a global classical solution $(u, v)$ which is {\bf bounded} in $Ω\times(0,+\infty)$. Moreover, if $μ$ is large enough, the solution $(u, v)$ exponentially converges to the constant stationary solution $(\frac{a}{μ}, \frac{a}{μ})$ in the norm of $L^\infty(Ω)$ as $t\rightarrow\infty$. To the best of our knowledge, this new result is {\bf the first} analytical work for the boundedness and {\bf asymptotic behavior} of Keller--Segel system with {\bf singular sensitivity} and {\bf logistic source} in higher dimension case ($N\geq3$).

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A new (and optimal) result for boundedness of solution of a quasilinear chemotaxis--haptotaxis model (with logistic source)

This article deals with an initial-boundary value problem for the coupled chemotaxis-haptotaxis system with nonlinear diffusion $$\left\{\begin{array}{ll} u_t=\nabla\cdot( D(u)\nabla u)-χ\nabla\cdot(u\nabla v)- ξ\nabla\cdot(u\nabla w)+μu(1- u-w), x\in Ω, t>0,\\ τv_t=Δv- v +u,\quad x\in Ω, t>0,\\ w_t=- vw,\quad x\in Ω, t>0, \end{array}\right.$$ under homogeneous Neumann boundary conditions in a smooth bounded domain $Ω\subset\mathbb{R}^N(N\geq1)$, where $τ\in\{0,1\}$ and $χ$, $ξ$ and $μ$ are given nonnegative parameters. As far as we know, this situation provides the first {\bf rigorous} result which (precisely) gives the relationship between $m,ξ,χ$ and $μ$ that yields to the boundedness of the solutions. Moreover, these results thereby significantly extending results of previous results of several authors (see Remarks 1.1 and 1.2) and some optimal results are obtained.

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Global existence, smooth and stabilization in a three-dimensional Keller-Segel-Navier-Stokes system with rotational flux

We consider the spatially $3$-D version of the following Keller-Segel-Navier-Stokes system with rotational flux $$\left\{\begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot(nS(x,n,c)\nabla c),\quad x\in Ω, t>0, c_t+u\cdot\nabla c=Δc-c+n,\quad x\in Ω, t>0,\\ u_t+κ(u \cdot \nabla)u+\nabla P=Δu+n\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0,\quad x\in Ω, t>0 \end{array}\right.\qquad(*)$$ under no-flux boundary conditions in a bounded domain $Ω\subseteq \mathbb{R}^{3}$ with smooth boundary, where $ϕ\in W^{2,\infty} (Ω)$ and $κ\in \mathbb{R}$ represent the prescribed gravitational potential and the strength of nonlinear fluid convection, respectively. Here the matrix-valued function $S(x,n,c)\in C^2(\barΩ\times[0,\infty)^2 ;\mathbb{R}^{3\times 3})$ denotes the rotational effect which satisfies $|S(x,n,c)|\leq C_S(1 + n)^{-α}$ with some $C_S > 0$ and $α\geq 0$. In this paper, by seeking some new functionals and using the bootstrap arguments on system $(*)$, we establish the existence of global weak solutions to system $(*)$ for arbitrarily large initial data under the assumption $α\geq1$. Moreover, under an explicit condition on the size of $C_S$ relative to $C_N$, we can secondly prove that in fact any such {\bf weak} solution $(n,c,u)$ becomes smooth ultimately, and that it approaches the unique spatially homogeneous steady state $(\bar{n}_0,\bar{n}_0,0)$, where $\bar{n}_0=\frac{1}{|Ω|}\int_Ωn_0$ and $C_N$ is the best Poincaré constant. To the best of our knowledge, there are the first results on asymptotic behavior of the system.

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A new result for 2D boundedness of solutions to a chemotaxis--haptotaxis model with/without sub-logistic source

We consider the Neumann problem for a coupled chemotaxis-haptotaxis model of cancer invasion with/without kinetic source in a 2D bounded and smooth domain. For a large class of cell kinetic sources including zero source and sub-logistic sources, we detect an explicit condition involving the chemotactic strength, the asymptotic "damping" rate, and the initial mass of cells to ensure uniform-in-time boundedness for the corresponding Neumann problem. Our finding significantly improves existing 2D global existence and boundedness in related chemotaxis-/haptotaxis systems.

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A new result for the global existence (and boundedness), regularity and stabilization of a three-dimensional Keller-Segel-Navier-Stokes system modeling coral fertilization

This paper deals with the following quasilinear Keller-Segel-Navier-Stokes system modeling coral fertilization $(*)$: $$\left\{ \begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot(nS(x,n,c)\nabla c)-nm,\quad x\in Ω, t>0, c_t+u\cdot\nabla c=Δc-c+m,\quad x\in Ω, t>0, m_t+u\cdot\nabla m=Δm-nm,\quad x\in Ω, t>0,\\ u_t+κ(u \cdot \nabla)u+\nabla P=Δu+(n+m)\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0,\quad x\in Ω, t>0 \end{array}\right.$$ under no-flux boundary conditions in a bounded domain $Ω\subset \mathbb{R}^3$ with smooth boundary, where $ϕ\in W^{2,\infty} (Ω)$. Here the matrix-valued function $S(x,n,c)$ denotes the rotational effect which satisfies $|S(x,n,c)|\leq S_0 (c)(1 + n)^{-α}$ with $α\geq0$ and some nonnegative nondecreasing function $S_0$. Based on this inequality and some carefully analysis, if $α>0$, then for any $κ\in\mathbb{R},$ system $(*)$ possesses a global weak solution for which there exists $T > 0$ such that $(n,c,m , u)$ is smooth in $Ω\times( T ,\infty)$. Furthermore, for any $p>1,$ this solution is uniformly bounded in with respect to the norm in $L^p(Ω)\times L^\infty(Ω) \times L^\infty(Ω)\times L^2 (Ω; \mathbb{R}^3)$. Building on this boundedness property and some other analysis, it can finally even be proved that in the large time limit, any such solution approaches the spatially homogeneous equilibrium $(\hat{n},\hat{m},\hat{m},0)$ in an appropriate sense, where $\hat{n}=\frac{1}{|Ω|}\{\int_Ωn_0-\int_Ωm_0\}_{+}$ and $\hat{m}=\frac{1}{|Ω|}\{\int_Ωm_0 -\int_Ωn_0\}_{+}$.

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Global weak solutions in a three-dimensional Keller-Segel-Navier-Stokes system modeling coral fertilization

We consider an initial-boundary value problem for the incompressible four-component Keller-Segel-Navier-Stokes system with rotational flux $$\left\{\begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot(nS(x,n,c)\nabla c)-nm,\quad x\in Ω, t>0,\\ c_t+u\cdot\nabla c=Δc-c+m,\quad x\in Ω, t>0,\\ m_t+u\cdot\nabla m=Δm-nm,\quad x\in Ω, t>0,\\ u_t+κ(u \cdot \nabla)u+\nabla P=Δu+(n+m)\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0,\quad x\in Ω, t>0 \end{array}\right.$$ in a bounded domain $Ω\subset \mathbb{R}^3$ with smooth boundary, where $κ\in \mathbb{R}$ is given constant, $S$ is a matrix-valued sensitivity satisfying $|S(x,n,c)|\leq C_S(1+n)^{-α}$ with some $C_S> 0$ and $α\geq 0$. As the case $κ= 0$ (with $α\geq\frac{1}{3}$ or the initial data satisfy a certain smallness condition) has been considered in [14], based on new gradient-like functional inequality, it is shown in the present paper that the corresponding initial-boundary problem with $κ\neq 0$ admits at least one global weak solution if $α>0$. To the best of our knowledge, this is the first analytical work for the {\bf full three-dimensional four-component} chemotaxis-Navier-Stokes system.

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Blow-up prevention by nonlinear diffusion in a 2D Keller-Segel-Navier-Stokes system with rotational flux

This paper investigates the following Keller-Segel-Navier-Stokes system with nonlinear diffusion and rotational flux $$\begin{align}\begin{cases} &n_t+u\cdot\nabla n=Δn^m-\nabla\cdot(nS(x, n, c)\nabla c),\quad &x\in Ω, t>0, \\ &c_t+u\cdot\nabla c=Δc-c+n,\quad &x\in Ω, t>0, \\ &u_t+κ(u\cdot\nabla)u+\nabla P=Δu+n\nabla ϕ,\quad &x\in Ω, t>0, \\ &\nabla\cdot u=0,\quad &x\in Ω, t>0, \end{cases}\end{align}$$ where $κ\in \mathbb{R},ϕ\in W^{2,\infty}(Ω)$ and $S$ is a given function with values in $\mathbb{R}^{2\times2}$ which fulfills $$ |S(x,n,c)| \leq C_S $$ with some $C _S > 0$. Systems of this type describe chemotaxis-fluid interaction in cases when the evolution of the chemoattractant is essentially dominated by production through cells. If $m>1$ and $Ω\subset \mathbb{R}^2$ is a {\bf bounded} domain with smooth boundary, then for all reasonably regular initial data, a corresponding initial-boundary value problem for $(KSNF)$ possesses a global and bounded (weak) solution, which significantly improves previous results of several authors. Moreover, the {\bf optimal condition} on the parameter $m$ for global existence is obtained. Our approach underlying the derivation of main result is based on an entropy-like estimate involving the functional %Our main tool is consideration of the energy functional $$\int_Ω(n_{\varepsilon} +\varepsilon)^{m}+\int_Ω|\nabla c_\varepsilon|^{2},$$ where $n_\varepsilon$ and $c_\varepsilon$ are components of the solutions to (2.1) below.

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An optimal result for global classical and bounded solutions in a two-dimensional Keller-Segel-Navier-Stokes system with sensitivity

This paper deals with a boundary-value problem for a coupled chemotaxis-Navier-Stokes system involving tensor-valued sensitivity with saturation $$\left\{ \begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot(nS(x,n,c)\nabla c),\quad x\in Ω, t>0, c_t+u\cdot\nabla c=Δc-c+n,\quad x\in Ω, t>0,\\ u_t+κ(u \cdot \nabla)u+\nabla P=Δu+n\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0,\quad x\in Ω, t>0, \end{array}\right.$$ which describes chemotaxis-fluid interaction in cases when the evolution of the chemoattractant is essentially dominated by production through cells, where $κ\in \mathbb{R},ϕ\in W^{2,\infty}(Ω)$ and $S$ is a given function with values in $\mathbb{R}^{2\times2}$ which fulfills $$|S(x,n,c)| \leq C_S (1 + n)^{-α}$$ with some $C _S > 0$ and $α\geq 0.$ If $α>0$ and $Ω\subseteq \mathbb{R}^2$ is a {\bf bounded} domain with smooth boundary, then for all reasonably regular initial data, a corresponding initial-boundary value problem for $(KSNF)$ possesses a global classical solution which is bounded on $Ω\times(0,\infty)$. This extends a recent result by Wang-Winkler-Xiang (Annali della Scuola Normale Superiore di Pisa-Classe di Scienze. XVIII, (2018), 2036--2145) which asserts global existence of bounded solutions under the constraint $Ω\subseteq \mathbb{R}^2$ is a bounded {\bf convex domain} with smooth boundary. Moreover, we shall improve the result of Wang-Xiang (J. Diff. Eqns., 259(2015), 7578--7609), who proved the possibility of global and bounded, in the case that ${\bfκ\equiv0}$ and $α>0$. In comparison to the result for the corresponding fluid-free system, the {\bf optimal condition} on the parameter $α$ for both {\bf global existence} and {\bf boundedness} are obtained.

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Boundedness of solution of a parabolic--ODE--parabolic chemotaxis--haptotaxis model with (generalized) logistic source

In this paper, we study the following chemotaxis--haptotaxis system with (generalized) logistic source $$ \left\{\begin{array}{ll} u_t=Δu-χ\nabla\cdot(u\nabla v)- ξ\nabla\cdot(u\nabla w)+u(a-μu^{r-1}-w), \displaystyle{v_t=Δv- v +u},\quad \\ \displaystyle{w_t=- vw},\quad\\ \displaystyle{\frac{\partial u}{\partial ν}=\frac{\partial v}{\partial ν}=\frac{\partial w}{\partial ν}=0},\quad x\in \partialΩ, t>0,\\ \displaystyle{u(x,0)=u_0(x)},v(x,0)=v_0(x),w(x,0)=w_0(x),\quad x\in Ω, \end{array}\right.\eqno(0.1) $$ %under homogeneous Neumann boundary conditions in a smooth bounded domain $\mathbb{R}^N(N\geq1)$, with parameter $r>1$. the parameters $a\in \mathbb{R}, μ>0, χ>0$. It is shown that when $r>2$, or \begin{equation*} μ>μ^{*}=\begin{array}{ll} \frac{(N-2)_{+}}{N}(χ+C_β) C^{\frac{1}{\frac{N}{2}+1}}_{\frac{N}{2}+1},~~~\mbox{if}~~r=2, \end{array} \end{equation*} % $μ>\frac{(N-2)_{+}}{N}χC^{\frac{1}{\frac{N}{2}+1}}_{\frac{N}{2}+1}$, the considered problem possesses a global classical solution which is bounded, where $C^{\frac{1}{\frac{N}{2}+1}}_{\frac{N}{2}+1}$ is a positive constant which is corresponding to the maximal sobolev regularity. Here $C_β$ is a positive constant which depends on $ξ$, $\|u_0\|_{C(\barΩ)},\|v_0\|_{W^{1,\infty}(Ω)}$ and $\|w_0\|_{L^\infty(Ω)}$. This result improves or extends previous results of several authors.

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A new result for boundedness in the quasilinear parabolic-parabolic Keller-Segel model (with logistic source)

The current paper considers the boundedness of solutions to the following quasilinear Keller-Segel model (with logistic source) $$\left\{\begin{array}{ll} u_t = \nabla\cdot(D(u)\nabla u)-χ\nabla\cdot(u\nabla v)+μ(u-u^2),\quad x\in Ω, t>0,\\ v_t-Δv = u-v,\quad x\in Ω, t>0,\\ (D(u)\nabla u-χu\cdot \nabla v)\cdot ν= \frac{\partial v}{\partialν}=0,\quad x\in \partialΩ, t>0,\\ u(x,0) = u_0(x),\quad v(x,0) = v_0(x),\ \ x\in Ω, \end{array}\right.$$ where $Ω\subset\mathbb{R}^N(N\geq1)$ is a bounded domain with smooth boundary $\partialΩ,$ $χ>0$ and $μ\geq0$. We prove that for nonnegative and suitably smooth initial data $(u_0, v_0)$, if $D(u)\geq C_{D}(u+1)^{m-1}$ for all $u\geq 0$ with some $C_{D} > 0$ and some $m>2-\frac{2}{N}\frac{χ\max\{1,λ_0\}}{[χ\max\{1,λ_0\}-μ]_{+}}$ or $m=2-\frac{2}{N}$ and $C_D>\frac{C_{GN}(1+\|u_0\|_{L^1(Ω)})}{3}(2-\frac{2}{N})^2\max\{1,λ_0\}χ$, the $(KS)$ possesses a global classical solution which is bounded in $Ω\times (0,\infty)$, where $C_{GN}$ and $λ_0$ are the constants which are corresponding to the Gagliardo--Nirenberg inequality and the maximal Sobolev regularity. To our best knowledge, this seems to be the first rigorous mathematical result which (precisely) gives the relationship between $m$ and $\fracμχ$ that yields to the boundedness of the solutions.

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An optimal result for global existence and boundedness in a three-dimensional Keller-Segel-Stokes system with nonlinear diffusion

This paper investigates the following quasilinear Keller-Segel-Navier-Stokes system $$\left\{ \begin{array}{l} n_t+u\cdot\nabla n=Δn^m-\nabla\cdot(n\nabla c),\quad x\in Ω, t>0, \\ c_t+u\cdot\nabla c=Δc-c+n,\quad x\in Ω, t>0,\\ u_t+\nabla P=Δu+n\nabla ϕ,\quad x\in Ω, t>0,\\ \nabla\cdot u=0, \quad x\in Ω, t>0 \end{array}\right.$$ under homogeneous boundary conditions of Neumann type for $n$ and $c$, and of Dirichlet type for $u$ in a three-dimensional bounded domains $Ω\subseteq \mathbb{R}^3$ with smooth boundary, where $ϕ\in W^{1,\infty}(Ω),m>0$. It is proved that if $m>\frac{4}{3}$, then for any sufficiently regular nonnegative initial data there exists at least one global boundedness solution for system $(KSF)$, which in view of the known results for the fluid-free system mentioned below (see Introduction) is an optimal restriction on $m$.

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An optimal result for global existence and boundedness in a three-dimensional Keller-Segel(-Navier)-Stokes system (involving a tensor-valued sensitivity with saturation)

The coupled quasilinear Keller-Segel-Navier-Stokes system $$ \left\{ \begin{array}{l} n_t+u\cdot\nabla n=Δn-\nabla\cdot(nS(x,n,c)\nabla c),\quad x\in Ω, t>0, c_t+u\cdot\nabla c=Δc-c+n,\quad x\in Ω, t>0, u_t+κ(u \cdot \nabla)u+\nabla P=Δu+n\nabla ϕ,\quad x\in Ω, t>0, \nabla\cdot u=0,\quad x\in Ω, t>0 \end{array}\right.\eqno(KSNF) $$ is considered under Neumann boundary conditions for $n$ and $c$ and no-slip boundary conditions for $u$ in three-dimensional bounded domains $Ω\subseteq \mathbb{R}^3$ with smooth boundary, where $κ\in \mathbb{R}$ is given constant, $ϕ\in W^{1,\infty}(Ω),m>0$, $|S(x,n,c)|\leq C_S(1+n)^{-α}$ and the parameter $α\geq0$. %For any small $μ>0$, If $α>\frac{1}{3}$, then for all reasonably regular initial data, a corresponding initial-boundary value problem for $(KSNF)$ possesses a globally defined weak solution. This result improves the result of Wang (Math. Models Methods Appl. Sci., 27(14):2745--2780, 2017), where the global {\bf very weak} solution for system $(KSNF)$ is obtained. Moreover, if $κ=0$ and $S(x,n,c)=C_S(1+n)^{-α}$, then the system $(KSF)$ exists at least one global classical solution which is bounded in $Ω\times(0,\infty)$. These results significantly improve or extend previous results of several authors. In comparison to the result for the corresponding fluid-free system, the {\bf optimal condition} on the parameter $α$ for global (weak) existence and boundedness is obtained. Our proofs rely on Maximal Sobolev regularity techniques and on a variant of the natural gradient-like energy functional.

math.AP

Global solvability and boundedness in the $N$-dimensional quasilinear chemotaxis model with logistic source and consumption of chemoattractant

We consider the following chemotaxis model %fully parabolic Keller-Segel system with logistic source $$ \left\{\begin{array}{ll} u_t=\nabla\cdot(D(u)\nabla u)-χ\nabla\cdot(u\nabla v)+μ(u-u^2),\quad x\in Ω, t>0, \disp{v_t-Δv=-uv },\quad x\in Ω, t>0, %\disp{τw_t+δw=u },\quad %x\in Ω, t>0, \disp{(\nabla D(u)-χu\cdot \nabla v)\cdot ν=\frac{\partial v}{\partialν}=0},\quad x\in \partialΩ, t>0, \disp{u(x,0)=u_0(x)},\quad v(x,0)=v_0(x),~~ x\in Ω\end{array}\right. $$ on a bounded domain $Ω\subset\mathbb{R}^N(N\geq1)$, with smooth boundary $\partialΩ, χ$ and $μ$ are positive constants. Besides appropriate smoothness assumptions, in this paper it is only required that $D(u)\geq C_{D}(u+1)^{m-1}$ for all $u\geq 0$ with some $C_{D} > 0$ and some $$ m>\left\{\begin{array}{ll} 1-\fracμ{χ[1+λ_{0}\|v_0\|_{L^\infty(Ω)}2^{3}]}~~\mbox{if}~~ N\leq2, % >1+\frac{(N+2-2r)^+}{N+2}~~~~~~\mbox{if}~~ % \frac{N+2}{2}\geq r\geq\frac{N+2}{N}, 1~~~~~~\mbox{if}~~ N\geq3, \end{array}\right. $$ then for any sufficiently smooth initial data there exists a classical solution which is global in time and bounded, where $λ_{0}$ is a positive constant which is corresponding to the maximal sobolev regularity. The results of this paper extends the results of Jin (J. Diff. Eqns., 263(9)(2017), 5759-5772), who proved the possibility of boundness of weak solutions, in the case $m>1$ and $N=3$.

math.AP