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Quasilinear parabolic problems with nonlinear boundary conditions

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Turning to (c), let g ∈ Ξi+1 and v ∈ Zi+1(V −1<br />

i g). Evidently hij (g, v) ∈ Zi+1. If i > 0,<br />

we further have<br />

h ij (g, v)| [0,Ti] = (L ij<br />

i+1 (ϕjg + k ∗ Cj(·, x, Dx)v))| [0,Ti]<br />

= L ij<br />

i (ϕjg| [0,Ti] + k ∗ Cj(·, x, Dx)V −1<br />

i<br />

= ϕjV −1<br />

i<br />

g − Lij<br />

i<br />

g) (here ∗ is meant on [0, Ti])<br />

k ∗ (Aj<br />

# (·, x, Dx) − A j<br />

# (Ti, xj, Dx))ϕjV −1<br />

i g.<br />

Thus, w ∈ Zi+1(ϕjV −1<br />

i g) implies F (w) := Sijw + hij (g, v) ∈ Zi+1(ϕjV −1<br />

i g). In fact,<br />

(F (w))| [0,Ti] = L ij<br />

i k ∗ (Aj # (·, x, Dx) − A j<br />

# (Ti, xj, Dx))ϕjV −1<br />

i g + hij (g, v)| [0,Ti]<br />

= ϕjV −1<br />

i g.<br />

So F is a self-mapping of Zi+1(ϕjV −1<br />

i g). This is true for i = 0, too. Compare the<br />

initial values of all terms occurring above to see this. In view of (4.17), F is also a strict<br />

contraction. Hence the assertion follows by the contraction principle. �<br />

4.2 Half space <strong>problems</strong><br />

This section is devoted to <strong>parabolic</strong> <strong>problems</strong> of second order in a half space subject<br />

to general <strong>boundary</strong> <strong>conditions</strong>. In the first subsection we study the case in which the<br />

coefficients are constant and the differential operators consist only of their principal<br />

parts. Then we shall prove pointwise multiplication properties for the function spaces<br />

arising as the natural regularity classes on the <strong>boundary</strong>. These results allow us to treat<br />

also the case of variable coefficients by means of perturbation arguments. This will be<br />

done in the last part of this paragraph.<br />

4.2.1 Constant coefficients<br />

Let J = [0, T ] and R n+1<br />

+ = {x := (x′ , y) ∈ R n+1 : x ′ ∈ R n , y > 0}. We separately<br />

consider the <strong>problems</strong><br />

� u − k ∗ a : ∇ 2 xu = f, t ∈ J, x ∈ R n+1<br />

+ ,<br />

u = g, t ∈ J, x ′ ∈ R n , y = 0,<br />

� u − k ∗ a : ∇ 2 xu = f, t ∈ J, x ∈ R n+1<br />

+ ,<br />

−∂yu + b · ∇x ′u = h, t ∈ J, x′ ∈ R n , y = 0,<br />

(4.18)<br />

(4.19)<br />

where k is as in Section 4.1, a is an (n + 1)-dimensional real matrix, and b ∈ R n . We<br />

look for unique solutions u in the maximal regularity space<br />

As to (4.18), we have the following result.<br />

Z := H α p (J; Lp(R n+1<br />

+ )) ∩ Lp(J; H 2 p(R n+1<br />

+ )).<br />

Theorem 4.2.1 Let 1 < p < ∞, n ∈ N, and a ∈ Sym{n + 1}. Let further k ∈ K 1 (α, θ),<br />

where θ < π and α ∈ (0, 2) \<br />

definite.<br />

� 1<br />

p , 2<br />

2p−1<br />

1 3<br />

, 1 + p , 1 + 2p−1<br />

63<br />

�<br />

. Assume that a is positive

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