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 + 2nε ≥ 2nε > 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
) = 2η∆η|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
≥ (2η∆η − 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
+2u∆u =
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 |Dφ|
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
(η∆η + 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
dened 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 dene 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
x∈B
1
|u(x) − u(x
0
)|
|x − x
0
|
α/2
≤ 2
α/2
sup
x∈∂B
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.
Dene K = sup
x∈∂B
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
.
Dene 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/2−2
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