In this work we extend a recent result to chemotaxis fluid systems which
include matrix-valued sensitivity functions
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&=\Delta n^m-\nabla!\cdot(nS(x,n,c)\nabla c),
&x\in\Omega,& t>0,\ c_{t}&+&u\cdot!\nabla c&=\Delta c-c+n,\ &x\in\Omega,&
t>0,\ u_{t}&+&(u\cdot\nabla)u&=\Delta u+\nabla P+n\nabla\phi,\ &x\in\Omega,&
t>0,\ &&\nabla\cdot u&=0,\ &x\in\Omega,& t>0, \end{array}\right. \end{align*}
in a bounded domain with smooth boundary. Assuming
that , satisfy , that the matrix-valued
function satisfies
for some 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 and , i.e. , we will establish the
existence of at least one global weak solution in the standard sense.

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