# Boundedness of the derivative of the trace of an H^1 function

As a research preface, this question is linked to a problem of increasing magnetism in Ginzburg-Landau equations that I have distilled for the purpose of getting to the bottom of this technical matter.

Suppose $u_n\in H^1(B_1)$ (actually, $u_n$ are smooth), where $B_1$ is the unit ball in $\mathbb{R}^N$, and that we know $||u_n||_{H^1} \leq C$, so that up to a subsequence, $u_n \rightharpoonup u$ in $H^1(B_1)$ weakly. What can we say about the boundedness of the quantity

$\int_{\partial B_1} \nabla u_n(x) \cdot n(x)\;d\mathcal{H}^{N-1}(x)$,

where $n(x)$ is the unit normal to $\partial B_1$?

In particular, is this quantity always finite under these hypotheses, or is there a counterexample that shows this blows up for a bounded subset of $H^1$?

• If you take $u_n(x) := n^{1/2} (|x|-1+\frac{1}{n})_+$, then the $u_n$ are bounded in $H^1$ but the integral blows up like $n^{1/2}$. Oct 3 '13 at 17:43

Clearly, what you call $\newcommand{\bn}{\boldsymbol{n}}$ $\nabla u\cdot \bn$ is the normal derivative $\frac{\partial u}{\partial \bn}$. The trace theorem (see e.g. Lions and Magenes, Non-Homogeneous Boundary Value Problems and Applications. I, Thm. 9.4, Chap 1) shows that for $s> \frac{3}{2}$ the restriction map $\newcommand{\pa}{\partial}$

$$R: C^\infty(B_1)\ni u\mapsto (u|_{\pa B_1}, \frac{\pa u}{\pa \bn})\in C^\infty(\pa B_1)\times C^\infty(\pa B_1)$$

extends to a continuous split surjective map

$$H^s(B_1)\to H^{s-\frac{1}{2}}(\pa B_1) \times H^{s-\frac{3}{2}}(\pa B_1).$$

The result is optimal because Theorem 9.5, Chap. 1 op. cit. shows that if $s\leq \frac{3}{2}$, then for any $\phi\in C^\infty(\pa B_1)$ the linear functional

$$C^\infty( B_1)\ni u\mapsto \int_{\pa B_1} \frac{\pa u (x)}{\pa \bn} \phi (x) dA(x)\in\mathbb{R}$$

is not continuous in the topology induced by $H^s(B_1)$. In particular, if $s\leq \frac{3}{2}$ there cannot exist a constant $C>0$ such that

$$\left|\int_{\pa B_1} \frac{\pa u}{\pa \bn} dA\right| \leq C\Vert u\Vert_{H^s(B_1)},\;\;\forall u\in C^\infty(B_1),$$

so that there exists a sequence $u_k\in C^\infty(B_1)$ such that $\Vert u_k\Vert_{H^1(B_1)}\leq 1$ and

$$\left|\int_{\pa B_1} \frac{\pa u_k}{\pa \bn} dA\right| \to \infty.$$

If you restrict a $H^s$-function $f$ to a submanifold of codimension $k$ you get a $H^{s-k/2}$ function.

EDIT: But only if $s$ is large enough (Sobolev lemma threshold). Thus the rest of my answer does not work, and I deleted it.

The second order term in your PDE is the Laplacian. Even though in $H^1$ you cannot define the trace on the boundary, the Laplacian helps. I am not sure of which particular problem you are thinking of (many things are called Ginzburg-Landau), but the Pohozaev identity usually helps. See for example 'Vortices in the Magnetic Ginzburg-Landau Model' Here by Sandier and Serfaty -where many references of its use are given. They show for example that for $$-\Delta u = \frac{u}{\epsilon^2}(1-|u|^2) \textrm{ in }\Omega$$ with $u=g$ on $\partial\Omega$, $|g|=1$ and $\Omega$ star-shaped, there holds (Lemma 5.2) $$\int_\Omega \frac{(1-|u|^2)^2}{\epsilon^2} + \int_{\partial \Omega} \left|\frac{\partial u}{\partial n}\right|^2 \leq C(\Omega,g),$$ So the normal derivative is $L^2(\partial\Omega)$, and this does not follow from $u\in H^1(\Omega)$.

The Pohozaev identity is to use as a test function $x\cdot \nabla u$ in the case of a ball, that is, a test function that will equal $\partial_n u$ on the boundary. This idea is also known under the name of Morawetz multiplier, and Rellich identity.