Math Notes

Record my math notes

Maximum Principles

Section 1.4: Maximum Principles
1.4 Maximum Principles
In this section we will use the maximum principle to derive the interior gradient
estimate and the Harnack inequality.
Theorem 1.29. Suppose u C
2
(B
1
) C(B
1
) is a subharmonic function in B
1
; that
is, u 0. Then there holds
sup
B
1
u sup
B
1
u.
Proof. For ε > 0 we consider u
ε
(x) = u(x) + ε|x|
2
in B
1
. Then simple calculation yields
u
ε
= u + 2 2 > 0.
It is easy to see, by a contradiction argument, that u
ε
cannot have an interior maximum,
in particular,
sup
B
1
u
ε
sup
B
1
u
ε
.
Therefore we have
sup
B
1
u sup
B
1
u
ε
sup
B
1
u + ε.
We nish the proof by letting ε 0.
Remark 1.30. The result still holds if B
1
is replaced by any bounded domain.
The next result is the interior gradient estimate for harmonic functions. The method
is due to Bernstein back in 1910.
Proposition 1.31. Suppose u is harmonic in B
1
. Then there holds
sup
B
1/2
|Du| c sup
B
1
|u|
where c = c(n) is a positive constant. In particular, for any α [0, 1] there holds
|u(x) u(y)| c|x y|
α
sup
B
1
|u| for any x, y B
1/2
where c = c(n, α) is a positive constant.
Proof. Direct calculation shows that
∆(|Du|
2
) = 2
n
X
i,j=1
(D
ij
u)
2
+ 2
n
X
i=1
D
i
uD
i
(∆u) = 2
n
X
i,j=1
(D
ij
u)
2
where we used u = 0 in B
1
. Hence |Du|
2
is a subharmonic function. To get interior
23
Chapter 1: Harmonic Functions
estimates we need a cuto function. For any φ C
1
0
(B
1
) we have
∆(φ|Du|
2
) = (∆φ)|Du|
2
+ 4
n
X
i,j
=1
D
i
φD
j
uD
ij
u + 2φ
n
X
i,j
=1
(D
ij
u)
2
.
By taking φ = η
2
for some η C
1
0
(B
1
) with η = 1 in B
1/2
, we obtain by the Hölder
inequality
∆(η
2
|Du|
2
) = 2ηη|Du|
2
+ 2|Dη|
2
|Du|
2
+ 8η
n
X
i,j=1
D
i
ηD
j
uD
ij
u + 2η
2
n
X
i,j=1
(D
ij
u)
2
(2ηη 6|Dη|
2
)|Du|
2
C| Du|
2
where C is a positive constant depending only on η. Note that ∆(u
2
) = 2|Du|
2
+2uu =
2|Du|
2
since u is harmonic. By taking α large enough we get
∆(η
2
|Du|
2
+ αu
2
) 0.
We may apply Theorem 1.29 (the maximum principle) to get the result.
Next we derive the Harnack inequality.
Lemma 1.32. Suppose u is a nonnegative harmonic function in B
1
. Then there holds
sup
B
1/2
|D log u| C
where C = C(n) is a positive constant.
Proof. We may assume u > 0 in B
1
. Set v = log u. Then direct calculation shows
v = −|Dv|
2
.
We need the interior gradient estimate on v. Set w = |Dv|
2
. Then we get
w + 2
n
X
i=1
D
i
vD
i
w = 2
n
X
i,j=1
(D
ij
v)
2
.
As before we need a cuto function. First note
n
X
i,j=1
(D
ij
v)
2
n
X
i=1
(D
ii
v)
2
1
n
(∆v)
2
=
|Dv|
4
n
=
w
2
n
. (1.6)
24
Section 1.4: Maximum Principles
Take a nonnegative function φ C
1
0
(B
1
). We obtain by the Hölder inequality
∆(φw) + 2
n
X
i
=1
D
i
vD
i
(φw) = 2φ
n
X
i,j
=1
(D
ij
v)
2
+ 4
n
X
i,j
=1
D
i
φD
j
vD
ij
v + 2w
n
X
i
=1
D
i
φD
i
v + (∆φ)w
φ
n
X
i,j=1
(D
ij
v)
2
2|Dφ||Dv|
3
|φ| + C
|Dφ|
2
φ
|Dv|
2
if φ is chosen such that ||
2
/φ is bounded in B
1
. Choose φ = η
4
for some η C
1
0
(B
1
).
Hence for such xed η we obtain by (1.1)
∆(
η
4
w
) + 2
n
X
i=1
D
i
vD
i
(
η
4
w
)
1
n
η
4
|Dv|
4
Cη
3
|Dη||Dv|
3
4η
2
(ηη + C|Dη|
2
)|Dv|
2
1
n
η
4
|Dv|
4
Cη
3
|Dv|
3
Cη
2
|Dv|
2
where C is a positive constant depending only on n and η. Hence we get by the Hölder
inequality
∆(η
4
w) + 2
n
X
i=1
D
i
vD
i
(η
4
w)
1
n
η
4
w
2
C
where C is a positive constant depending only on n and η. Suppose η
4
w attains its
maximum at x
0
B
1
. Then D(η
4
w) = 0 and ∆(η
4
w) 0 at x
0
. Hence there holds
η
4
w
2
(x
0
) C(n, η).
If w(x
0
) 1, then η
4
w(x
0
) C(n). Otherwise η
4
w(x
0
) w(x
0
) η
4
(x
0
). In both
cases we conclude
η
4
w C(n, η) in B
1
.
Corollary 1.33. Suppose u is a nonnegative harmonic function in B
1
. Then there holds
u(x
1
) Cu(x
2
) for any x
1
, x
2
B
1/2
where C is a positive constant depending only on n.
Proof. We may assume u > 0 in B
1
. For any x
1
, x
2
B
1/2
by simple integration we
obtain with Lemma 1.32
log
u(x
1
)
u(x
2
)
|x
1
x
2
|
Z
1
0
|D log u(tx
2
+ (1 t)x
1
)|dt C|x
1
x
2
|.
25
Chapter 1: Harmonic Functions
Next we prove a quantitative Hopf lemma.
Proposition 1.34. Suppose u C(B
1
) is a harmonic function in B
1
= B
1
(0). If
u(x) < u(x
0
) for any x B
1
and some x
0
B
1
, then there holds
u
n
(x
0
) C(u(x
0
) u(0))
where C is a positive constant depending only on n.
Proof. Consider a positive function v in B
1
dened by
v(x) = e
α|x|
2
e
α
.
It is easy to see
v(x) = e
α|x|
2
(2αn + 4α
2
|x|
2
) > 0 for any |x|
1
2
if α 2n + 1 . Hence for such xed α the function v is subharmonic in the region
A = B
1
\ B
1/2
. Now dene for ε > 0
h
ε
(x) = u(x) u(x
0
) + εv(x).
This is also a subharmonic function, that is, h
ε
0 in A. Obviously h
ε
0 on
B
1
and h
ε
(x
0
) = 0. Since u(x) < u(x
0
) for |x| =
1
2
we may take ε > 0 small such
that h
ε
(x) < 0 for |x| =
1
2
. Therefore by Theorem 1.29 h
ε
assumes at the point x
0
its
maximum in A. This implies
h
ε
n
(x
0
) 0 or
u
n
(x
0
) ε
v
n
(x
0
) = 2αεe
α
> 0.
Note that so far we have only used the subharmonicity of u. We estimate ε as follows.
Set w(x) = u(x
0
) u(x) > 0 in B
1
. Obviously w is a harmonic function in B
1
. By
Corollary 1.33 (the Harnack inequality) there holds
inf
B
1/2
w c(n)w(0) or max
B
1/2
u u(x
0
) c(n)(u(x
0
) u(0)).
Hence we may take
ε = δc(n)(u(x
0
) u(0))
for δ small, depending on n. This nishes the proof.
To nish this section we prove a global Hölder continuity result.
Lemma 1.35. Suppose u C(B
1
) is a harmonic function in B
1
with u = φ on B
1
. If
26
Section 1.4: Maximum Principles
φ C
α
(B
1
) for some α (0, 1), then u C
α/2
(B
1
). Moreover, there holds
kuk
C
α/2
(B
1
)
Ckφk
C
α
(B
1
)
where C is a positive constant depending only on n and α.
Proof. First the maximum principle implies that inf
B
1
φ u sup
B
1
φ in B
1
. Next
we claim that for any x
0
B
1
there holds
sup
xB
1
|u(x) u(x
0
)|
|x x
0
|
α/2
2
α/2
sup
xB
1
|φ(x) φ(x
0
)|
|x x
0
|
α
. (1.7)
Lemma 1.35 follows easily from (1.7). For any x, y B
1
, set d
x
= dist(x, B
1
) and
d
y
= dist(y, B
1
). Suppose d
y
d
x
. Take x
0
, y
0
B
1
such that |x x
0
| = d
x
and
|y y
0
| = d
y
. Assume rst that |x y| d
x
/2.
Then y
¯
B
d
x
/2
(x) B
d
x
(x) B
1
. We apply Proposition 1.31 (scaled version) to
u u(x
0
) in B
d
x
(x) and get by (1.7)
d
α/2
x
|u(x) u(y)|
|x y|
α/2
Cku u(x
0
)k
L
(B
d
x
(x))
Cd
α/2
x
kφk
C
α
(B
1
)
.
Hence we obtain
|u(x) u(y)| C|x y|
α/2
kφk
C
α
(B
1
)
.
Assume now that d
y
d
x
2|x y|. Then by (1.7) again we have
|u(x) u(y)| |u(x) u(x
0
)| + |u(x
0
) u(y
0
)| + |u(y
0
) u(y)|
C(d
α/2
x
+ |x
0
y
0
|
α/2
+ d
α/2
y
)kφk
C
α
(B
1
)
C|x y|
α/2
kφk
C
α
(B
1
)
since |x
0
y
0
| d
x
+ |x y| + d
y
5|x y|.
In order to prove (1.7) we assume B
1
= B
1
((1, 0, . . . , 0)), x
0
= 0, and φ(0) = 0.
Dene K = sup
xB
1
|φ(x)|/|x|
α
. Note |x|
2
= 2x
1
for x B
1
. Therefore for x B
1
there holds
φ(x) K|x|
α
2
α/2
Kx
α/2
1
.
Dene v(x) = 2
α/2
Kx
α/2
1
in B
1
. Then we have
v(x) = 2
α/2
K ·
α
2
α
2
1
x
α/22
1
< 0 in B
1
.
Theorem 3.1 implies
u(x) v(x) = 2
α/2
Kx
α/2
1
2
α/2
K|x|
α/2
for any x B
1
.
27
Chapter 1: Harmonic Functions
Considering u similarly, we get
|u(x)| 2
α/2
K|x|
α/2
for any x B
1
.
This proves (1.7).
28
0%