In
mathematics, there is in
mathematical analysis a class of
Sobolev inequalities, relating norms including those of
Sobolev spaces. These are used to prove the
Sobolev embedding theorem, giving inclusions between certain
Sobolev spaces, and the
Kondrashov theorem (or
Rellich-Kondrashov theorem) showing that under slightly stronger conditions some Sobolev spaces are
compactly embedded in others. They are named after
Sergei Lvovich Sobolev.
Sobolev embedding theorem
Let
Wk,p(
Rn) denote the Sobolev space consisting of all real-valued functions on
Rn whose first
k weak derivatives are functions in
Lp. Here
k is a non-negative integer and 1 ≤
p ≤ ∞. The first part of the Sobolev embedding theorem states that
if
k >
ℓ and 1 ≤
p <
q ≤ ∞ are two extended real numbers such that:
then
and the embedding is continuous. In the special case of
k = 1 and
ℓ = 0, Sobolev embedding gives
where
p∗ is the
Sobolev conjugate of
p, given by
This special case of the Sobolev embedding is a direct consequence of the
Gagliardo–Nirenberg–Sobolev inequality.
The second part of the Sobolev embedding theorem applies to embeddings in
Hölder spaces
Cr,α(
Rn). If (
k−
r−α)/
n > 1/
p with α ∈ (0,1), then one has the embedding
This part of the Sobolev embedding is a direct consequence of
Morrey's inequality.
Generalizations
The Sobolev embedding theorem holds for Sobolev spaces
Wk,p(
M) on other suitable domains
M. In particular (; ), both parts of the Sobolev embedding hold when
Kondrashov embedding theorem
On a compact manifold with
C1 boundary, the
Kondrashov embedding theorem states that if
k>
ℓ and
k−
n/
p >
ℓ−
n/
q then the Sobolev embedding
is
completely continuous (compact).
Gagliardo–Nirenberg–Sobolev inequality
Assume that
u is a continuously differentiable real-valued function on
Rn with
compact support. Then for 1 ≤
p <
n there is a constant
C depending only on
n and
p such that
where
is the
Sobolev conjugate of
p.
The Gagliardo–Nirenberg–Sobolev inequality implies directly the Sobolev embedding
The embeddings in other orders on
Rn are then obtained by suitable iteration.
Hardy–Littlewood–Sobolev lemma
Sobolev's original proof of the Sobolev embedding theorem relied on the following, sometimes known as the Hardy–Littlewood–Sobolev
fractional integration theorem. An equivalent statement is known as the
Sobolev lemma in . A proof is in .
Let 0 < α <
n and 1 <
p < ∞. Let
Iα = (−Δ)
−α/2 be the
Riesz potential on
Rn. Then, for
q defined by
there exists a constant
C depending only on
p such that
If
p = 1, then the weak-type estimate holds:
where 1/
q = 1 − α/
n.
The Hardy–Littlewood–Sobolev lemma implies the Sobolev embedding essentially by the relationship between the
Riesz transforms and the Riesz potentials.
Morrey's inequality
Assume
n <
p ≤ ∞. Then there exists a constant
C, depending only on
p and
n, such that
for all
u ∈ C
1(
Rn) ∩ L
p(
Rn), where
Thus if
u ∈
W1,p(
Rn), then
u is in fact
Hölder continuous of exponent γ,
after possibly being redefined on a set of measure 0.
A similar result holds in a bounded domain
U with
C1 boundary. In this case,
where the constant
C depends now on
n,
p and
U. This version of the inequality follows from the previous one by applying the norm-preserving extension of
W1,p(
U) to
W1,p(
Rn).
General Sobolev inequalities
Let
U be a bounded open subset of
Rn, with a
C1 boundary. (
U may also be unbounded, but in this case its boundary, if it exists, must be sufficiently well-behaved.) Assume
u ∈
Wk,p(
U).
(i) If
then
, where
We have in addition the estimate
,
the constant
C depending only on
k,
p,
n, and
U.
(ii) If
then
u belongs to the
Hölder space , where
if n/p is not an integer, or
γ is any positive number < 1, if n/p is an integer
We have in addition the estimate
the constant
C depending only on
k,
p,
n, γ, and
U.
Case
If
, then
is a function of
bounded mean oscillation and
This estimate is a corollary of the
Poincaré inequality.
Nash inequality
The Nash inequality, introduced by , states that there exists a constant
C > 0, such that for all
u ∈ L
1(
Rn) ∩ W
1,2(
Rn),
The inequality follows from basic properties of the
Fourier transform. On the one hand, integrating over the complement of the ball of radius ρ,
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by
Parseval's theorem. On the other hand, one has
which, when integrated over the ball of radius ρ gives
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where ω
n is the volume of the
n-ball. Choosing ρ to minimize the sum of () and () and again applying Parseval's theorem
gives the inequality.
In the special case of
n =1, the Nash inequality can be extended to the
Lp case, in which case it is a generalization of the Gagliardo-Nirenberg-Sobolev inequality . In fact, if
I is a bounded interval, then for all 1 ≤
r < ∞ and all 1 ≤
q ≤
p < ∞ the following inequality holds
where
a is defined by