Quasilinear parabolic problems with nonlinear boundary conditions
Quasilinear parabolic problems with nonlinear boundary conditions
Quasilinear parabolic problems with nonlinear boundary conditions
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3.3 More time regularity for Volterra equations<br />
This section deals <strong>with</strong> the question under what <strong>conditions</strong> the solution of equation (3.1)<br />
lies in the space<br />
H α+κ<br />
p (J; X) ∩ H κ p (J; DA),<br />
where, in contrast to Section 3.1, we assume κ ∈ (1/p, 1 + 1/p) and α + κ < 2 + 1/p.<br />
Theorem 3.3.1 Let X be a Banach space of class HT , p ∈ (1, ∞), J a compact timeinterval<br />
[0, T ], and A an R-sectorial operator in X <strong>with</strong> R-angle φR A . Suppose that a<br />
belongs to K1 (α, θa) <strong>with</strong> α ∈ (0, 2). Further let κ ∈ (1/p, 1 + 1/p), α + κ < 2 + 1/p and<br />
α + κ �= 1 + 1/p. Assume the <strong>parabolic</strong>ity condition θa + φR A < π. Then (3.1) has a<br />
unique solution in Z := Hα+κ p (J; X) ∩ Hκ p (J; DA) if and only if<br />
(i) f(0) ∈ D(A);<br />
(ii) f = h + (1 ∗ a)Af(0), <strong>with</strong> h ∈ H α+κ<br />
p<br />
case α + κ > 1 + 1/p.<br />
(J; X), and ˙ h(0) ∈ DA(1 + κ 1 1<br />
α − α − pα , p) in<br />
Proof. We first show the necessity part. Suppose that u ∈ Z solves (3.1). Then, κ > 1/p<br />
entails α + κ > 1/p. Thus, the trace x := u(0) ∈ X exists. Furthermore we see that<br />
Au ∈ C(J; X). So, by the closedness of A, x ∈ D(A) and we infer from (3.1) that<br />
u(t) + (a ∗ A(u − x))(t) = f(t) − (1 ∗ a)(t)Ax, t ∈ J.<br />
From A(u − x) ∈ 0H κ p (J; X), it follows that a ∗ A(u − x) ∈ 0H α+κ<br />
p (J; X), in view of<br />
Corollary 2.8.1. In addition, 1 ∗ a is absolutely continuous on J and vanishes at t = 0.<br />
Hence, f(0) = x as well as f = h+(1∗a)Af(0), where h is defined by h = u+a∗A(u−x) ∈<br />
Hα+κ p (J; X). This proves (i) and the first part of (ii).<br />
To verify the second condition in (ii), suppose that α + κ > 1 + 1/p. Owing to<br />
a ∗ A(u − x) ∈ 0H α+κ<br />
p (J; X), we have ˙ h(0) = ˙u(0). We now consider two cases. In<br />
case of κ ∈ (1/p, 1), we can argue as in the proof of Theorem 3.1.4, Case 3, to see that<br />
˙u(0) ∈ DA(1 + κ/α − 1/α − 1/pα, p). If κ ∈ [1, 1 + 1/p), then<br />
˙u ∈ H α+κ−1<br />
p<br />
(J; X) ∩ H κ−1<br />
p (J; DA),<br />
and we obtain the desired regularity of ˙u(0) <strong>with</strong> the aid of Theorem 3.1.4, applied to<br />
the equation<br />
˙u(t) + (a ∗ A ˙u)(t) = g(t), t ∈ J,<br />
<strong>with</strong> some g ∈ Hα+κ−1 p (J; X). Hence, the necessity part is complete.<br />
We now want to prove the converse. Uniqueness follows immediately from Theorem<br />
3.1.1. Concerning sufficiency, we suppose validity of (i) and (ii) and distinguish two<br />
cases.<br />
If α+κ < 1+1/p, we set u = x+u1, where u1 is defined as solution of v+a∗Av = h−x<br />
on J. Condition (i) ensures that the constant function w(t) = x, t ∈ J lies in Z. From<br />
the second condition, we deduce h(0) = f(0) = x and h − x ∈ 0H α+κ<br />
p (J; X). So, due to<br />
Remark 3.1.1(ii), we obtain u1 ∈ 0H α+κ<br />
p (J; X) ∩ 0H κ p (J; DA). Thus u ∈ Z. Further,<br />
u + a ∗ Au = (x + (1 ∗ a)Ax) + (h − x) = f,<br />
by condition (ii). Hence, u ∈ Z is indeed the solution of (3.1).<br />
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