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Quasilinear parabolic problems with nonlinear boundary conditions

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Remarks 3.1.2 (i) It is not difficult to see that the second assertion of Theorem 3.1.2<br />

remains true if we allow κ to lie in [1/p, 1 + 1/p).<br />

(ii) Let κ = 0, A be invertible, and assume that the kernel a admits in addition the<br />

estimate C ≤ s −α |â(s)|, s > 0, for some constant C > 0. Then by taking J = R+ in the<br />

above lines and by employing this additional estimate, one obtains the implications<br />

x ∈ DA(1 − 1<br />

pα , p) ⇒ S(·)x ∈ Lp(R+; DA), if α > 1<br />

p ;<br />

y ∈ DA(1 − 1 1<br />

α − pα , p) ⇒ (1 ∗ S)(·)y ∈ Lp(R+; DA), if α > 1 + 1<br />

p ,<br />

see also Prüss [64, Theorem 6].<br />

(iii) The proof of Theorem 3.1.2 is inspired by the estimates derived in the proof of<br />

Theorem 6 in Prüss [64].<br />

We next want to show that these <strong>conditions</strong> on the traces are also necessary. In the<br />

following theorem, again, the operator A is only sectorial. For technical reasons, we<br />

have to assume maximal regularity of the solutions of (3.4) and (3.5), respectively, on<br />

the whole halfline. Later on we shall extend this result to <strong>problems</strong> on compact timeintervals<br />

where the operator A is R-sectorial.<br />

Theorem 3.1.3 Let X be a Banach space of class HT , p ∈ (1, ∞), and A a sectorial<br />

operator in X <strong>with</strong> spectral angle φA. Suppose that κ ∈ [0, 1/p), a ∈ K 1 (α, θa) <strong>with</strong><br />

α ∈ (1/p − κ, 2), α + κ �= 1 + 1/p. Further let ω ≥ 0 and assume that θa + φA < π. Then<br />

and if α + κ > 1 + 1/p,<br />

e−ω· AS(·)x ∈ Hκ p (R+; X) ⇒ x ∈ DA(1 + κ 1<br />

α − pα , p), (3.11)<br />

e−ω· A(1 ∗ S)(·)y ∈ Hκ p (R+; X) ⇒ y ∈ DA(1 + κ 1 1<br />

α − α − pα , p). (3.12)<br />

Proof. The main idea of the proof is to use Proposition 1 in [64], which says that for<br />

every function g in Lp(R+; X), the Laplace transform ˆg(λ) exists for Re λ > 0, and <strong>with</strong><br />

p −1 + q −1 = 1 the estimate<br />

� ∞<br />

0<br />

|ˆg(λ)| p λ p−2 dλ ≤ |g| p<br />

Lp(R+;X) Γ(1/q)p<br />

(3.13)<br />

holds true.<br />

We first show implication (3.11). Let Bκ be defined as in the proof of Theorem<br />

3.1.2. Suppose that g(t) := Bκ(e −ωt AS(t)x), t ≥ 0, is contained in Lp(R+; X). Then<br />

g is Laplace transformable, according to the proposition mentioned above. From the<br />

resolvent equation for S(·), S(t)x + (a ∗ AS)(t)x = x, t ≥ 0, it follows by the convolution<br />

theorem that<br />

ˆg(λ) = λκ<br />

λ + ω A(1 + âω(λ)A) −1 x, Re λ > 0.<br />

Here, aω(t) := a(t)e −ωt , t ≥ 0. Therefore, using (3.13) we obtain<br />

� ∞<br />

η := ( λ1+κ− 1<br />

p<br />

λ + ω |A(1 + âω(λ)A) −1 p dλ<br />

x|X) ≤ C|g|p<br />

λ Lp(R+;X) . (3.14)<br />

0<br />

From Lemma 2.6.2 we know that aω ∈ K 1 (α, θa). So, in similar manner as in the proof<br />

of Theorem 3.1.2, we can derive the following estimate from the resolvent equation for<br />

A and <strong>parabolic</strong>ity of (3.4):<br />

|A(|λ| α + A) −1 x| ≤ (C1 + C2(|âω(λ)| |λ| α ) −1 ) |A(1/âω(λ) + A) −1 x|, Re λ > 0,<br />

39

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