3.4 Green Potentials 129
where 0 <<1andc
0
> 1. The set {(x, y, z); u(x, y, z) >} is a neighbor-
hood of (0, 0, 0) and the set {(x, y, z); u(x, y, z) < 1+c
0
} is an open set which
excludes the line segment {(x, 0, 0); 0 <x<1}. It is easily seen that
lim
|(x,y,z)|→0
u(x, y, z)=1− lim
|(x,y,z)|→0
x log ρ
2
where ρ
2
= y
2
+ z
2
.If(x, y, z) → (0, 0, 0) along a path for which x>0,y
2
+
z
2
=0andx
k
= ρ
2
for some positive integer k,thenu(x, y, z) → 1; note
also that such points will be in Ω if sufficiently close to (0, 0, 0). If, however,
(x, y, z) → (0, 0, 0) along a path for which x>0,y
2
+ z
2
=0andρ =
exp (−c/2x)withc>c
0
,thenu(x, y, z) → 1+c; note also that such points
will be in ∼ Ω if sufficiently close to (0, 0, 0). It follows that (0, 0, 0) is a
boundary point for Ω. It remains only to show that (0, 0, 0) is an irregular
boundary point for the region Ω. The function u, as the Newtonian potential
of a measure with compact support, is harmonic on the open set Ω. As such,
it is the solution of the Dirichlet problem for the boundary function which is
equal to on the boundary of the region u>and equal to 1 + c
0
on the
boundary of the region u<1+c
0
.Forx<0,
u(x, 0, 0) =
1
0
ξ
ξ − x
dξ =1+x log (1 − x) −x log |x|
so that lim
x→0−
u(x, 0, 0) = 1 < 1+c
0
.
In general, little can be said about the continuity of a Green potential
G
Ω
μ unless the measure μ is absolutely continuous with respect to Lebesgue
measure. If Ω is a Greenian set and f is a measurable function on Ω,let
G
Ω
f(x)=
Ω
G
Ω
(x, y)f(y) dy
provided the integral is defined for all x ∈ Ω.
Theorem 3.4.12 If Ω is a Greenian set and f is a bounded Lebesgue inte-
grable function on Ω,thenG
Ω
f is continuous on Ω.
Proof: Since the positive and negative parts f
+
and f
−
areintegrableover
Ω and G
Ω
f = G
Ω
f
+
− G
Ω
f
−
, it can be assumed that 0 ≤ f ≤ m for some
constant m. By Theorem 3.4.4, G
Ω
f is a potential. Let B = B
y,ρ
be a ball
with B
−
⊂ Ω of radius less that 1/2. Then G
Ω
f = G
Ω
fχ
B
+ G
Ω
fχ
Ω∼B
.
Since the density fχ
Ω∼B
assigns zero measure to B,G
Ω
fχ
Ω∼B
is harmonic
on B by Theorem 3.4.7 and therefore continuous on B.ConsidernowG
Ω
fχ
B
.
If it can be shown that G
Ω
fχ
B
is continuous on B ∼{y}, it would follow that
G
Ω
f is continuous on B ∼{y}; but since B = B
y,ρ
is an arbitrary ball with
closure in Ω, this would imply that G
Ω
f is continuous on Ω.SinceG
Ω
fχ
B
differs from G
B
f by a function harmonic on B by Theorem 3.4.8, it suffices
to prove that G
B
f is continuous on B ∼{y}. It is necessary to consider the