CONCENTRATING SOLUTIONS FOR A PLANAR ... - CAPDE
CONCENTRATING SOLUTIONS FOR A PLANAR ... - CAPDE
CONCENTRATING SOLUTIONS FOR A PLANAR ... - CAPDE
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33<br />
where δ lj denotes the Kronecker’s symbol, and hence, we get that<br />
|<br />
2∑<br />
k=1 l=1<br />
m∑<br />
∫<br />
c kl<br />
Ω<br />
≤ C‖φ ξ ‖ ∞ max |c kl |<br />
k , l<br />
[∂ (ξj ) i<br />
(e U l<br />
Z kl<br />
)<br />
+ η(x − ξ j )∂ xi<br />
(e U l<br />
Z kl<br />
)]<br />
φ ξ |<br />
∫<br />
Ω<br />
(<br />
)<br />
e U l<br />
+ O(e − 3 4 p ) = O( 1 p 7 )<br />
in view of |Z 0l Z kl | ≤ 2, (4.5)-(4.6). Inserting in (5.8), we get that<br />
∫<br />
Ω<br />
(<br />
∆u ξ + u p )<br />
ξ<br />
∂ (ξj ) i<br />
φ ξ = −<br />
2∑<br />
k=1 l=1<br />
+O( 1 p 7 ).<br />
m∑<br />
∫<br />
c kl<br />
Ω<br />
e U l<br />
Z kl ∂ xi (η(x − ξ j )φ ξ )(5.9)<br />
Since pφ ξ → 0 in C 1 -norm away from ξ 1 , . . . , ξ m , (5.9) gives that<br />
∫<br />
Ω<br />
( )<br />
∆u ξ + u p ξ<br />
∂ (ξj ) i<br />
φ ξ = −<br />
= −<br />
2∑<br />
k=1 l=1<br />
∫<br />
m∑<br />
∫<br />
c kl<br />
B(ξ j ,ɛ)<br />
always in view of (4.1) and (4.5)-(4.6).<br />
B(ξ j ,ɛ)<br />
(<br />
∆u ξ + u p ξ<br />
e U l<br />
Z kl ∂ xi φ ξ + O( 1 p 7 )<br />
)<br />
∂ xi φ ξ + O( 1 p 7 ) (5.10)<br />
Now, by Lemma 2.1 we get that | 1 δ s<br />
∂ xi w l ( x−ξs<br />
δ s<br />
)| ≤ C for any l = 1, 2 and<br />
for x away from ξ s . Hence, by the expression of U ξ and (2.2), (2.11) we get<br />
that for |x − ξ j | ≤ 2ɛ:<br />
m∑<br />
(<br />
1<br />
∂ xi U ξ =<br />
2<br />
∂ xi P U δs ,ξ s<br />
+ 1 (<br />
p−1<br />
p ∂ x i<br />
P w 0 ( x − ξ )<br />
s<br />
)<br />
(5.11)<br />
δ<br />
s=1 γµ<br />
s<br />
s<br />
+ 1 (<br />
p 2 ∂ x i<br />
P w 1 ( x − ξ ))<br />
s<br />
)<br />
δ s<br />
m∑<br />
(<br />
1<br />
=<br />
2<br />
∂ xi U δs,ξs + 1 ∂ xi w 0 ( x − ξ s<br />
) + 1<br />
p−1<br />
pδ<br />
s=1 γµ<br />
s δ s p 2 ∂ xi w 1 ( x − ξ )<br />
s<br />
) + O( 1 δ s δ s γ )<br />
s<br />
(<br />
1<br />
= −<br />
2<br />
Z ij − 1<br />
p−1 p ∂ x i<br />
w 0 ( x − ξ j<br />
) − 1 δ<br />
γδ j µ<br />
j p 2 ∂ x i<br />
w 1 ( x − ξ )<br />
j<br />
) + O( 1 δ j γ ),<br />
j<br />
since ∂ xi U δs ,ξ s<br />
= − 1 δ s<br />
Z is . Since, as already observed, ∂ xi w l ( x−ξ j<br />
δ j<br />
) = O(δ j )<br />
uniformly away from ξ j , l = 1, 2, by (5.11) in particular we get:<br />
∂ xi U ξ = O( 1 ), (5.12)<br />
γ