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(FG 4)
Cooperation with: V. Maz'ya (Linköping University, Sweden)
Description: The reported work continues efforts to prove existence, uniqueness, and regularity results for elliptic and parabolic equations and systems which describe phenomena in physics, chemistry, and biology (see Annual Research Reports 2000 p. 19 et sqq. and 2002 p. 39 et sqq.). In particular, we are interested in quasilinear systems of the form
which comprise--among others--reaction-diffusion systems and heat conduction, see [1] or [4] and the references cited therein. The focus is on the case of spatially three-dimensional nonsmooth domains and discontinuous coefficients , which occur in modeling
heterogeneous media. 
Over the past years various tools
for the study of such equations have been developed at the
Weierstrass Institute, see [13,
14, 15, 19].  
In particular, the result of
Gröger [15] is  of great use in many applications, see
[2, 4, 7, 
11, 18] to name only a
few. Gröger's result states that
is a topological isomorphism for 
q
, which occur in modeling
heterogeneous media. 
Over the past years various tools
for the study of such equations have been developed at the
Weierstrass Institute, see [13,
14, 15, 19].  
In particular, the result of
Gröger [15] is  of great use in many applications, see
[2, 4, 7, 
11, 18] to name only a
few. Gröger's result states that
is a topological isomorphism for 
q  ]2, q0[ in case of Lipschitz
domains, (elliptic) L
 ]2, q0[ in case of Lipschitz
domains, (elliptic) L coefficient functions, and mixed
boundary conditions.  Unfortunately, it is well known that 
in
general q0 exceeds 2 only slightly. 
Thus, in view of
embedding theorems generically only the case of two space dimensions
is covered. However, 
for many applications it is not sufficient to study only equations
in two space dimensions, that means physical systems which are--in
one space direction--translational or circular invariant, see, e.g.,
[2] or [9].
The increasing structural complexity
of technical devices requires to perform
simulations and the corresponding mathematical analysis on 
three-dimensional domains, see 
[10, 16].
 coefficient functions, and mixed
boundary conditions.  Unfortunately, it is well known that 
in
general q0 exceeds 2 only slightly. 
Thus, in view of
embedding theorems generically only the case of two space dimensions
is covered. However, 
for many applications it is not sufficient to study only equations
in two space dimensions, that means physical systems which are--in
one space direction--translational or circular invariant, see, e.g.,
[2] or [9].
The increasing structural complexity
of technical devices requires to perform
simulations and the corresponding mathematical analysis on 
three-dimensional domains, see 
[10, 16].
In our recent paper [22] we 
study the Dirichlet problem for  (1) 
with 
piecewise constant coefficients  in a
polyhedral domain
 in a
polyhedral domain 
 
  
  .
We 
give conditions 
under which the problem
admits a unique solution from a space
.
We 
give conditions 
under which the problem
admits a unique solution from a space
 ;
; ))
))  C1((T0, T], Lp(
 C1((T0, T], Lp( ;
; )).
)).
 is a Lipschitz
polyhedron, that means
 is a Lipschitz
polyhedron, that means  is a bounded Lipschitz domain with
piecewise plane boundary. Furthermore, we assume that
 is a bounded Lipschitz domain with
piecewise plane boundary. Furthermore, we assume that  is the
union of a finite number of Lipschitz polyhedra
 is the
union of a finite number of Lipschitz polyhedra  , ...,
, ...,
 such that the 
(3 x 3) matrix functions
 such that the 
(3 x 3) matrix functions  are
constant on these subdomains.  The dependence of the functions Rk
on
 are
constant on these subdomains.  The dependence of the functions Rk
on 
 u is not stronger than quadratic.
                                The main advantage of our approach in comparison to the concept of
weak solutions is the strong differentiability of the solution
 with
respect to time and that the divergence of the corresponding currents
jk =
u is not stronger than quadratic.
                                The main advantage of our approach in comparison to the concept of
weak solutions is the strong differentiability of the solution
 with
respect to time and that the divergence of the corresponding currents
jk =  Jk(t,u)
Jk(t,u) uk are functions, not only
distributions. In a strict sense, only this justifies the application
of Gauss' theorem to calculate the normal components of the currents
over boundaries of (suitable) subdomains.
                                Our main result, [22, Theorem 6.10], ensures the
continuity of the normal fluxes across interfaces.
                                This property is also very important 
in the numerical analysis of finite volume
methods for heterostructures.
uk are functions, not only
distributions. In a strict sense, only this justifies the application
of Gauss' theorem to calculate the normal components of the currents
over boundaries of (suitable) subdomains.
                                Our main result, [22, Theorem 6.10], ensures the
continuity of the normal fluxes across interfaces.
                                This property is also very important 
in the numerical analysis of finite volume
methods for heterostructures.
The local existence result for (1) rests upon the classical
theorem of Sobolevskii on abstract quasilinear parabolic equations in
Banach spaces and estimates for elliptic transmission problems.
                                The problem is to find an adequate function space with respect to which the
hypotheses of Sobolevskii's theorem can be verified.
In the three-dimensional case one has to ensure 
that the linear operators in (2)
are topological isomorphisms for some q > 3, if the matrices
 =
 =  in (1) are piecewise constant. The operator
(2) corresponds to an interface (or transmission) problem
for the Laplacian, 
with different anisotropic materials given on the
polyhedral subdomains
 in (1) are piecewise constant. The operator
(2) corresponds to an interface (or transmission) problem
for the Laplacian, 
with different anisotropic materials given on the
polyhedral subdomains  , ...,
, ...,  of
 of  , with
Dirichlet conditions given on
, with
Dirichlet conditions given on 

 .
.
In contrast to the pure Laplacian on a Lipschitz
domain, see [17, Theorem 0.5], the gradients of
solutions to the transmission problems only belong to
L2+ for some
 for some 
 > 0. In the vicinity of
vertices and edges,
 > 0. In the vicinity of
vertices and edges, 
 may be arbitrarily small, even for
polygonal interface problems with only four isotropic
materials meeting in a vertex, see [20]. 
In the case of complex material coefficients,
which corresponds to some special anisotropy, even two materials
can produce strong singularities near vertices (see  
[5, 6], where similar problems are studied for
Helmholtz equations).
Therefore, a
large part of our investigation, [22], is devoted to
the optimal regularity for (2). This result inherently
applies to elliptic systems describing heterostructures on 
three-dimensional domains.
 may be arbitrarily small, even for
polygonal interface problems with only four isotropic
materials meeting in a vertex, see [20]. 
In the case of complex material coefficients,
which corresponds to some special anisotropy, even two materials
can produce strong singularities near vertices (see  
[5, 6], where similar problems are studied for
Helmholtz equations).
Therefore, a
large part of our investigation, [22], is devoted to
the optimal regularity for (2). This result inherently
applies to elliptic systems describing heterostructures on 
three-dimensional domains.
It is well known that the singularities of solutions to elliptic boundary value problems near vertices and edges can be characterized in terms of the eigenvalues of certain polynomial operator pencils on domains of the unit sphere or the unit circle. We refer to [21] for the case of the Dirichlet and Neumann problem and to [12] for the polyhedral Laplace interface problem with two isotropic materials. The corresponding analysis for several anisotropic materials has not been performed so far and is the subject of our investigation in [22].
To avoid the cumbersome analysis of optimal regularity near vertices, see [3], we use the somewhat surprising fact that if the solution of the interface problem belongs to Lq for some q > 3 near each interior point of the interface and boundary edges, then the operator (2) is an isomorphism. Thus, the regularity result for (2) can be reduced to that for an interface problem on dihedral angles with one common edge. The proof relies essentially on sharp pointwise estimates of Green's function, which we perform in [22].
The main result of our linear regularity theory is that the operator
(2) is an isomorphism for some q > 3 provided that
a  parameter 
 , which depends on
the decomposition of
, which depends on
the decomposition of  into the subdomains
 into the subdomains  , 
satisfies the inequality
, 
satisfies the inequality
 and the coefficient
and the coefficient  , or equivalently, on the
eigenvalues of certain pencils of ordinary differential operators.
These conditions can be checked for many heterostructures of practical
interest.  Though at this point our results are restricted to
Dirichlet boundary conditions, it should be possible to extend the
result to mixed boundary conditions, which occur, e.g., in modeling
semiconductor devices ([8]).  This problem will be
investigated in 2004.
, or equivalently, on the
eigenvalues of certain pencils of ordinary differential operators.
These conditions can be checked for many heterostructures of practical
interest.  Though at this point our results are restricted to
Dirichlet boundary conditions, it should be possible to extend the
result to mixed boundary conditions, which occur, e.g., in modeling
semiconductor devices ([8]).  This problem will be
investigated in 2004.
References:
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