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5.14. Proposition. Let 1 < p < ∞. Assume that the paths of symmetric matrices A(±∞, ·)<br />
satisfy the assumptions of Theorem 5.9. Then<br />
∂A : X 1,p<br />
S ,V ,V ′(Σ,�n ) → X p<br />
S (Σ,�n )<br />
is semi-Fredholm with ind∂A := dimker∂A − dimcoker∂A < +∞.<br />
Proof. We claim that there exist c ≥ 0 and s ≥ 0 such that, for any u ∈ X 1,p<br />
S ,V ,V ′(Σ,�n ), there<br />
holds<br />
�u�X1,p (Σ) ≤ c � �<br />
�(∂ + A)u�Xp (Σ) + �χsu�X p (Σ) , (97)<br />
where χs is the characteristic function of the set {z ∈ Σ | |Re z| ≤ s}.<br />
By Theorem 5.11 (ii), the asymptotic operators<br />
∂ + A(−∞, ·) : W 1,p<br />
(Σ,�n ) → L p (Σ,�n ),<br />
N ∗V0,N ∗V ′<br />
0<br />
∂ + A(+∞, ·) : W 1,p<br />
N ∗Vk,N ∗V ′<br />
k ′<br />
p<br />
(Σ,�n<br />
) → L (Σ,�n<br />
),<br />
are invertible. Since invertibility is an open condition in the operator norm, there exist s ><br />
max |Re S | + 2 and c1 > 0 such that for any u ∈ X 1,p<br />
S ,V ,V ′(Σ,�n ) with support disjoint from<br />
{|Rez| ≤ s − 1} there holds<br />
�u� X 1,p (Σ) = �u� W 1,p (Σ) ≤ c1�(∂ + A)u� L p (Σ) = c1�(∂ + A)u� X p (Σ). (98)<br />
By Proposition 5.10, there exists c2 > 0 such that for every u ∈ X 1,p<br />
S ,V ,V ′(Σ,�n ) with support in<br />
{|Rez| ≤ s} there holds<br />
�u� X 1,p (Σ) ≤ c2(�u� X p (Σ) + �∂u� X p (Σ))<br />
≤ (c2 + �A�∞)�u� X p (Σ) + c2�(∂ + A)u� X p (Σ).<br />
The inequality (97) easily follows from (98) and (99) by writing any u ∈ X 1,p<br />
S ,V ,V ′(Σ,�n ) as<br />
u = (1 − ϕ)u + ϕu, for ϕ a smooth real function on Σ having support in {|Re z| < s} and such<br />
that ϕ = 1 on {|Re z| ≤ s − 1}.<br />
Finally, by Proposition 5.13 the linear operator<br />
X 1,p<br />
S ,V ,V ′(Σ,�n ) → X p<br />
S (Σ,�n ), u ↦→ χsu,<br />
is compact. Therefore the estimate (97) implies that ∂A has finite dimensional kernel and closed<br />
range, that is it is semi-Fredholm with index less than +∞.<br />
It would not be difficult to use the regularity of weak solutions of the Cauchy-Riemann operator<br />
to prove that the cokernel of ∂A is finite-dimensional, so that ∂A is Fredholm. However, this will<br />
follow directly from the index computation presented in the next section.<br />
5.5 A Liouville type result<br />
Let us consider the following particular case in dimension n = 1:<br />
k = 1, k ′ = 0, S = {0}, V0 = (0), V1 =Ê, V ′<br />
0 =Ê, A(z) = α,<br />
with α a real number. In other words, we are looking at the operator ∂ +α on a space of�-valued<br />
maps u on Σ such that u(s) is purely imaginary for s ≤ 0, u(s) is real for s ≥ 0, and u(s + i) is<br />
real for every s ∈Ê. Notice that Φ − (t) = Φ + (t) = e iαt , so<br />
e iα iÊ∩Ê=(0) ∀α ∈Ê\(π/2 + π�), e iαÊ∩Ê=(0) ∀α ∈Ê\π�,<br />
so the assumptions of Theorem 5.9 are satisfied whenever α is not an integer multiple of π/2. In<br />
order to simplify the notation, we set<br />
X p (Σ) := X p<br />
{0} (Σ,�), X 1,p (Σ) := X 1,p<br />
{0},((0),Ê),(Ê) (Σ,�).<br />
We start by studying the regularity of the elements of the kernel of ∂α:<br />
63<br />
(99)