Gagliardo-Nirenberg-Sobolev inequality #
In this file we prove the Gagliardo-Nirenberg-Sobolev inequality.
This states that for compactly supported C¹
-functions between finite dimensional vector spaces,
we can bound the L^p
-norm of u
by the L^q
norm of the derivative of u
.
The bound is up to a constant that is independent of the function u
.
Let n
be the dimension of the domain.
The main step in the proof, which we dubbed the "grid-lines lemma" below, is a complicated
inductive argument that involves manipulating an n+1
-fold iterated integral and a product of
n+2
factors. In each step, one pushes one of the integral inside (all but one of)
the factors of the product using Hölder's inequality. The precise formulation of the induction
hypothesis (MeasureTheory.GridLines.T_insert_le_T_lmarginal_singleton
) is tricky,
and none of the 5 sources we referenced stated it.
In the formalization we use the operation MeasureTheory.lmarginal
to work with the iterated
integrals, and use MeasureTheory.lmarginal_insert'
to conveniently push one of the integrals
inside. The Hölder's inequality step is done using ENNReal.lintegral_mul_prod_norm_pow_le
.
The conclusions of the main results below are an estimation up to a constant multiple.
We don't really care about this constant, other than that it only depends on some pieces of data,
typically E
, μ
, p
and sometimes also the codomain of u
or the support of u
.
We state these constants as separate definitions.
Main results #
MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_eq
: The bound holds for1 ≤ p
,0 < n
andq⁻¹ = p⁻¹ - n⁻¹
MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_le
: The bound holds when1 ≤ p < n
,0 ≤ q
andp⁻¹ - n⁻¹ ≤ q⁻¹
. Note that in this case the constant depends on the support ofu
.
Potentially also useful:
MeasureTheory.eLpNorm_le_eLpNorm_fderiv_one
: this is the inequality forq = 1
. In this version, the codomain can be an arbitrary Banach space.MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_eq_inner
: in this version, the codomain is assumed to be a Hilbert space, without restrictions on its dimension.
The grid-lines lemma #
The "grid-lines operation" (not a standard name) which is central in the inductive proof of the Sobolev inequality.
For a finite dependent product Π i : ι, A i
of sigma-finite measure spaces, a finite set s
of
indices from ι
, and a (later assumed nonnegative) real number p
, this operation acts on a
function f
from Π i, A i
into the extended nonnegative reals. The operation is to partially
integrate, in the s
co-ordinates, the function whose value at x : Π i, A i
is obtained by
multiplying a certain power of f
with the product, for each co-ordinate i
in s
, of a certain
power of the integral of f
along the "grid line" in the i
direction through x
.
We are most interested in this operation when the set s
is the universe in ι
, but as a proxy for
"induction on dimension" we define it for a general set s
of co-ordinates: the s
-grid-lines
operation on a function f
which is constant along the co-ordinates in sᶜ
is morally (that is, up
to type-theoretic nonsense) the same thing as the universe-grid-lines operation on the associated
function on the "lower-dimensional" space Π i : s, A i
.
Equations
Instances For
The main inductive step in the grid-lines lemma for the Gagliardo-Nirenberg-Sobolev inequality.
The grid-lines operation GridLines.T
on a nonnegative function on a finitary product type is
less than or equal to the grid-lines operation of its partial integral in one co-ordinate
(the latter intuitively considered as a function on a space "one dimension down").
Auxiliary result for the grid-lines lemma. Given a nonnegative function on a finitary product
type indexed by ι
, and a set s
in ι
, consider partially integrating over the variables in
sᶜ
and performing the "grid-lines operation" (see GridLines.T
) to the resulting function in the
variables s
. This theorem states that this operation decreases as the number of grid-lines taken
increases.
The "grid-lines lemma" (not a standard name), stated with a general parameter p
as the
exponent. Compare with lintegral_prod_lintegral_pow_le
.
For any finite dependent product Π i : ι, A i
of sigma-finite measure spaces, for any
nonnegative real number p
such that (#ι - 1) * p ≤ 1
, for any function f
from Π i, A i
into
the extended nonnegative reals, we consider an associated "grid-lines quantity", the integral of an
associated function from Π i, A i
into the extended nonnegative reals. The value of this function
at x : Π i, A i
is obtained by multiplying a certain power of f
with the product, for each
co-ordinate i
, of a certain power of the integral of f
along the "grid line" in the i
direction through x
.
This lemma bounds the Lebesgue integral of the grid-lines quantity by a power of the Lebesgue
integral of f
.
Special case of the grid-lines lemma lintegral_mul_prod_lintegral_pow_le
, taking the extremal
exponent p = (#ι - 1)⁻¹
.
The Gagliardo-Nirenberg-Sobolev inequality #
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on ℝⁿ
, for n ≥ 2
. (More literally we encode ℝⁿ
as
ι → ℝ
where n := #ι
is finite and at least 2.) Then the Lebesgue integral of the pointwise
expression |u x| ^ (n / (n - 1))
is bounded above by the n / (n - 1)
-th power of the Lebesgue
integral of the Fréchet derivative of u
.
For a basis-free version, see lintegral_pow_le_pow_lintegral_fderiv
.
The constant factor occurring in the conclusion of lintegral_pow_le_pow_lintegral_fderiv
.
It only depends on E
, μ
and p
.
It is determined by the ratio of the measures on E
and ℝⁿ
and
the operator norm of a chosen equivalence E ≃ ℝⁿ
(raised to suitable powers involving p
).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n ≥ 2
, equipped
with Haar measure. Then the Lebesgue integral of the pointwise expression
|u x| ^ (n / (n - 1))
is bounded above by a constant times the n / (n - 1)
-th power of the
Lebesgue integral of the Fréchet derivative of u
.
The constant factor occurring in the conclusion of eLpNorm_le_eLpNorm_fderiv_one
.
It only depends on E
, μ
and p
.
Equations
Instances For
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n ≥ 2
, equipped
with Haar measure. Then the Lᵖ
norm of u
, where p := n / (n - 1)
, is bounded above by
a constant times the L¹
norm of the Fréchet derivative of u
.
Alias of MeasureTheory.eLpNorm_le_eLpNorm_fderiv_one
.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n ≥ 2
, equipped
with Haar measure. Then the Lᵖ
norm of u
, where p := n / (n - 1)
, is bounded above by
a constant times the L¹
norm of the Fréchet derivative of u
.
The constant factor occurring in the conclusion of eLpNorm_le_eLpNorm_fderiv_of_eq_inner
.
It only depends on E
, μ
and p
.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n
, equipped
with Haar measure, let 1 ≤ p < n
and let p'⁻¹ := p⁻¹ - n⁻¹
.
Then the Lᵖ'
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a Hilbert space.
Alias of MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_eq_inner
.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n
, equipped
with Haar measure, let 1 ≤ p < n
and let p'⁻¹ := p⁻¹ - n⁻¹
.
Then the Lᵖ'
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a Hilbert space.
The constant factor occurring in the conclusion of eLpNorm_le_eLpNorm_fderiv_of_eq
.
It only depends on E
, F
, μ
and p
.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n
, equipped
with Haar measure, let 1 < p < n
and let p'⁻¹ := p⁻¹ - n⁻¹
.
Then the Lᵖ'
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
This is the version where the codomain of u
is a finite dimensional normed space.
Alias of MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_eq
.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
compactly-supported function u
on a normed space E
of finite dimension n
, equipped
with Haar measure, let 1 < p < n
and let p'⁻¹ := p⁻¹ - n⁻¹
.
Then the Lᵖ'
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
This is the version where the codomain of u
is a finite dimensional normed space.
The constant factor occurring in the conclusion of eLpNorm_le_eLpNorm_fderiv_of_le
.
It only depends on F
, μ
, s
, p
and q
.
Equations
- MeasureTheory.eLpNormLESNormFDerivOfLeConst F μ s p q = let p' := (p⁻¹ - (↑(Module.finrank ℝ E))⁻¹)⁻¹; (μ s).toNNReal ^ (1 / ↑q - 1 / ↑p') * MeasureTheory.SNormLESNormFDerivOfEqConst F μ ↑p
Instances For
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
function u
supported in a bounded set s
in a normed space E
of finite dimension
n
, equipped with Haar measure, and let 1 < p < n
and 0 < q ≤ (p⁻¹ - (finrank ℝ E : ℝ)⁻¹)⁻¹
.
Then the L^q
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a finite dimensional normed space.
Alias of MeasureTheory.eLpNorm_le_eLpNorm_fderiv_of_le
.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
function u
supported in a bounded set s
in a normed space E
of finite dimension
n
, equipped with Haar measure, and let 1 < p < n
and 0 < q ≤ (p⁻¹ - (finrank ℝ E : ℝ)⁻¹)⁻¹
.
Then the L^q
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a finite dimensional normed space.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
function u
supported in a bounded set s
in a normed space E
of finite dimension
n
, equipped with Haar measure, and let 1 < p < n
.
Then the Lᵖ
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a finite dimensional normed space.
Alias of MeasureTheory.eLpNorm_le_eLpNorm_fderiv
.
The Gagliardo-Nirenberg-Sobolev inequality. Let u
be a continuously differentiable
function u
supported in a bounded set s
in a normed space E
of finite dimension
n
, equipped with Haar measure, and let 1 < p < n
.
Then the Lᵖ
norm of u
is bounded above by a constant times the Lᵖ
norm of
the Fréchet derivative of u
.
Note: The codomain of u
needs to be a finite dimensional normed space.