II.8 The Normed Dual of D
m,q
0
(Ω). The Spaces D
−m,q
0
113
We would like to analyze some significant consequences of this result for
the space D
1,q
0
(Ω). We begin to observe that, si nce D
1,q
0
(Ω) ⊂
˙
D
1,q
(Ω), by
Theorem I I.8.2 the generic linear functional on D
1,q
0
(Ω) can be represented
as in (II.8.11), for all u ∈ D
1,q
0
(Ω), where the function f ∈ [L
q
0
(Ω)]
n
is
determined up to a function f
0
such that
(f
0
, ∇u) = 0 , for all u ∈ D
1,q
0
(Ω) . (II.8.16)
Let
e
L
q
0
(Ω) be the subspace of [L
q
0
(Ω)]
n
constituted by all those functions
satisfying (II.8.16). It is immediately verified that
e
L
q
0
(Ω) is cl osed. Moreover,
setting G
0,q
0
(Ω) = M(D
1,q
0
0
(Ω)), with M defined in (II.8.13), we can readily
show that G
0,q
0
(Ω) is also a cl osed subspace of [L
q
0
(Ω)]
n
; see Exercise II.8.1.
Now, let f ∈ [L
q
0
(Ω)]
n
and consider the problem:
Find w ∈ D
1,q
0
0
(Ω) such that (∇w − f, ∇u) = 0 , for all u ∈ D
1,q
0
(Ω).
(II.8.17)
If Ω and f are sufficiently smooth, we can show that this problem is equivalent
to the following classical Dirichlet problem
∆w = ∇ ·f in Ω , w = 0 at ∂Ω , w ∈ D
1,q
0
0
(Ω) .
Lemma II.8.2 Assume that, for any given f ∈ [L
q
0
(Ω)]
n
, problem (II.8.17)
has one and only one solution w ∈ D
1,q
0
0
(Ω). Then, the fol lowing decomposi-
tion holds
[L
q
0
(Ω)]
n
=
e
L
q
0
(Ω) ⊕ G
0,q
0
(Ω) . (II.8.18)
Conversely, if (II.8.18) holds, then, for any f ∈ [L
q
0
(Ω)]
n
, problem (II.8.17)
is uniquely solvable. Finally, the linear o perator Π
q
0
: f ∈ [L
q
0
(Ω)]
n
→ f
1
∈
G
0,q
0
(Ω) is a projection (that is, Π
2
q
0
= Π
q
0
) and is continuous.
Proof. The last statement in the lemma is a consequence of (II.8.18); see
Rudin (1973, Theorem 5.16(b)). Since both L
q
0
(Ω) and G
0,q
0
(Ω) are closed,
in order to prove (II.8.18), under the given assumptio n, we have to show
that (a) L
q
0
(Ω) ∩ G
0,q
0
(Ω) = {0}, and that (b) f = f
0
+ f
1
, f
0
∈
e
L
q
0
(Ω),
f
1
∈ G
0,q
0
(Ω). Suppose there are l ∈
e
L
q
0
(Ω) and g = ∇ g ∈ G
0,q
0
(Ω), for
some g ∈ D
1,q
0
0
(Ω), such that l = g. This means, by definition of
e
L
q
0
(Ω)
that (∇g, ∇u) = 0 fo r all u ∈ D
1,q
0
(Ω), which, in turn, by the uni queness
assumption on problem (II.8.17), impli es ∇g = l = 0. Thus, (a) is proved.
Next, for the given f , let w ∈ D
1,q
0
(Ω) be the corresponding solution to
(II.8.17) and set f
0
= f − ∇w (∈
e
L
q
0
(Ω)), and f
1
= ∇w (∈ G
0,q
0
). Then,
f = f
0
+ f
1
which proves (b). The converse claim, namely, that (II.8.18)
implies the unique solvability of (II.8.17), is almost o bvious and, therefore, it
is l eft to the reader as an exercise ut