3.3 Symmetry of the Green Function 117
over Λ, which is unique. Since u
∞,Λ
will be considered only when a harmonic
minorant exists, further discussion is not warranted.
Lemma 3.3.6 If u
1
,u
2
are superharmonic on the open set Ω and have har-
monic minorants on Ω, then the greatest harmonic minorant of u
1
+u
2
exists
and is the sum of the greatest harmonic minorants of u
1
and u
2
.
Proof: Let {B
j
} be a sequence of balls and let {u
j
} be the corresponding
sequence of superharmonic functions defining u
∞
. Since the Poisson integral
is linear in the boundary function, (u
1
+ u
2
)
j
=(u
1
)
j
+(u
2
)
j
. Therefore,
(u
1
+ u
2
)
∞
=(u
1
)
∞
+(u
2
)
∞
and the lemma follows from Theorem 3.3.5.
Theorem 3.3.7 If the open set Ω is Greenian, then the greatest harmonic
minorant of G
Ω
(x, ·),x∈ Ω, is the zero function.
Proof: It is known that G
Ω
(x, ·) ≥ 0onΩ and that G
Ω
(x, ·) is superharmonic
on Ω. By Theorem 3.3.5, G
Ω
(x, ·) has a greatest harmonic minorant, since
the zero function is a harmonic function. Let h
x
be a harmonic minorant of
G
Ω
(x, ·). Then G
Ω
(x, ·) − h
x
≥ 0 and it can be written as the sum of u
x
and a harmonic function; that is, G
Ω
(x, ·) − h
x
∈B
x
. Therefore, G
Ω
(x, ·) ≤
G
Ω
(x, ·)−h
x
by the minimality of G
Ω
(x, ·). This shows that h
x
≤ 0andthat
the zero function is the greatest harmonic minorant of G
Ω
(x, ·).
The following theorem is a classic version of the domination principle
(c.f.Theorem 4.4.8).
Theorem 3.3.8 Let Ω be a Greenian subset of R
n
.Ifx ∈ Ω, Λ is a neigh-
borhood of x with compact closure in Ω,andu is a positive superharmonic
function defined on a neighborhood of Ω ∼ Λ with u ≥ G
Ω
(x, ·) on a neigh-
borhood of ∂Λ,thenu ≥ G
Ω
(x, ·) on Ω ∼ Λ.
Proof: Letting
w =
G
Ω
(x, ·)onΛ
min (G
Ω
(x, ·),u)onΩ ∼ Λ,
w is superharmonic on Ω.IfG
Ω
(x, ·) − w is defined to be 0 at x,then
it is a subharmonic minorant of G
Ω
(x, ·)onΩ. By Lemma 3.3.3 and the
fact that the greatest harmonic minorant of G
Ω
(x, ·) is the zero function,
G
Ω
(x, ·) − w ≤ 0sothatu ≥ G
Ω
(x, ·)onΩ ∼ Λ.
The method used to define u
∞,Λ
will be used to prove that the Green
function is a symmetric function of its arguments. The proof will require a
modification of the sequence of balls {B
j
} so that
∞
j=1
∂B
j
is closed relative
to Ω. Such a sequence can be constructed as follows. Let {Ω
k
} be a sequence
of open sets with compact closures such that Ω
k
↑ Ω and Ω
−
k
⊂ Ω, k ≥ 1. It
is easily seen using compactness arguments that there is a sequence of balls
{B
j
} such that only a finite number of balls intersect any Ω
−
k
. If the sequence
is modified so that each ball occurs infinitely often in the sequence, then this
will still be true. Suppose now that {x
i
} is a sequence in
∞
j=1
∂B
j
with