420 11 Oblique Derivative Problem
the {w
j
} sequence that converges uniformly on U ∩ (Ω ∪ Σ) to a function
w ∈ C
0
(cl(U ∩ Ω)) ∩C
2
(U ∩ (Ω ∪ Σ)) with Lw = f on U ∩ Ω and Mw = g
on U ∩Σ.Sincew ≤ inf {v
j
; j ≥ 1} on U ∩ Ω, w ≤ u on U ∩Ω and therefore
w = u on U ∩Ω.Thus,u ∈ C
0
(cl(U ∩Ω))∩C
2
(U ∩(Ω∪Σ)), Lu = f on U ∩Ω,
and Mu = g on U ∩Σ.Sincey and U are arbitrary, u ∈ C
2
(Ω ∪Σ), Lu = f
on Ω,andMu = g on Σ.
The following theorem is proved in the same way by using Lemma 11.4.7
in place of Lemma 11.4.5.
Theorem 11.4.13 If Σ = ∂Ω,β · ν ≥ >0 for some >0,c ≤ 0
on Ω, γ ≤ 0 on Σ,andν has a continuous extension to Σ
−
,thenu =
inf {v; v ∈ U(f,g,h)}∈C
0
b
(Ω)∩C
2
(Ω∪Σ), Lu = f on Ω,andMu = g on Σ.
As in Section 9.7, the function u =sup{w; w ∈ L(f,g,h)} will be called
the Perron subsolution and the corresponding v =inf{w : w ∈ U(f,g,h)}
the Perron supersolution. These two functions will be denoted by H
−
f,g,h
and H
+
f,g,h
, respectively. If H
+
f,g,h
= H
−
f,g,h
,thenh is said to be (L, M)-
resolutive and the common value is denoted by H
f,g,h
.Ifitcanbeshown
that lim
y→x,y∈Ω
H
±
f,g,h
(y)=h(x) for all x ∈ ∂Ω ∼ Σ, then it would follow
from Theorems 11.4.12, 11.4.13, and the strong maximum principle, Corol-
lary 11.3.6, that H
+
f,g,h
= H
−
f,g,h
on Ω and that h is (L, M)-resolutive. As in
the classical case, it is a question of finding conditions under which points
of ∂Ω ∼ Σ are regular boundary points. As was the case in Section 9.7, ap-
proximate barriers will be used to answer this question. As before, a region
Ω ⊂ R
n
will be called (L, M)-regular if lim
y→x,y∈Ω
H
f,g,h
(y)=h(x) for all
x ∈ ∂Ω ∼ Σ and all h ∈ C
0
(∂Ω ∼ Σ).
11.5 Regularity of Boundary Points
It was shown in Theorem 2.6.29 that the existence of a cone C ⊂∼ Ω with
vertex at x ∈ ∂Ω implies that x is a regular boundary point for the Dirichlet
problem u =0onΩ and u = g on ∂Ω. More generally, it was shown in
Theorem 9.8.8 that the existence of such a cone implies that x is a regular
boundary point for the elliptic boundary value problem Lu = f on Ω and
u = g on ∂Ω. The boundary behavior of a solution to the oblique derivative
problem Lu = f on Ω, Mu = g on Σ,andu = h on ∂Ω ∼ Σ is more
complicated. The behavior of u at points x ∈ Σ is determined by the existence
theorems, Theorems 11.4.12 and 11.4.13, which assert that u ∈ C
2
(Ω ∪ Σ)
and Mu = g on Σ.Forpointsx ∈ ∂Ω ∼ Σ, it is necessary to distinguish two
cases:
(i) x ∈ ∂Ω ∼ Σ,d(x, Σ) > 0
(ii) x ∈ ∂Ω ∼ Σ,d(x, Σ)=0.