SLIDE 1 On Hardy’s and Caffarelli, Kohn, Nirenberg’s inequalites.
S´ eminaire EDP-Analyse de l’Institut Camille Jordan, Lyon, April 2019
Hoai-Minh Nguyen
´ Ecole Polytechnique F´ ed´ erale de Lausanne EPFL, Switzerland joint with Marco Squassina
SLIDE 2 Outline
1 Known results related to Hardy’s and Caffarelli, Kohn,
Nirenberg’s (CKN’s) inequalities
2 CKN’s inequalities for fractional Sobolev spaces 3 New perspectives of Hardy’s and CKN’s inequalities in
Sobolev spaces.
SLIDE 3
Section 1: Known results related to Hardy’s and CKN’s inequalities
SLIDE 4 Hardy’s inequalities
1 For 1 p < d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd). 2 For p > d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd \ {0}). 3 For p = d > 1, ....
Standard proof is based on integration by parts.
SLIDE 5 Hardy’s inequalities
1 For 1 p < d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd). 2 For p > d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd \ {0}). 3 For p = d > 1, ....
Standard proof is based on integration by parts.
SLIDE 6 Hardy’s inequalities
1 For 1 p < d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd). 2 For p > d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd \ {0}). 3 For p = d > 1, ....
Standard proof is based on integration by parts.
SLIDE 7 Hardy’s inequalities
1 For 1 p < d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd). 2 For p > d,
ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
∀ u ∈ C1
c(Rd \ {0}). 3 For p = d > 1, ....
Standard proof is based on integration by parts.
SLIDE 8 Caffarelli, Kohn, Nirenberg’s inequalities, CM 84
Let p 1, q 1, τ > 0, 0 < a 1, α, β, γ ∈ R. One has
|x|γuLτ(Rd) C|x|α∇ua
Lp(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd)
under the following conditions 1
τ + γ d = a 1 p + α − 1 d
1 q + β d
with γ = aσ + (1 − a)β, 0 α − σ and
if 1
τ + γ d = 1 p + α − 1 d
and 1
τ + γ d,
1
p + α d,
1
q + β d > 0.
SLIDE 9 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 10 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 11 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 12 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 13 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 14 Comments on the CKN inequality
- This inequality is related to Gagliardo-Nirenberg’s inequality
when α = β = γ = 0, Gagliardo RM 59, Nirenberg ASNSP 59.
- A full story of Gagliardo-Nirenberg’s inequality for fractional
Sobolev spaces is due to Brezis and Mironescu AIHP 18.
- The proof of CKN’s inequality is based on
Integration by parts and symmetrization in the case 0 α − σ 1. Interpolation & the application of the previous case when
α − σ > 1 and 1
τ + γ d = 1 p + α−1 d
- CKN’s inequality generalizes Hardy’s inequality when 1 < p < d.
SLIDE 15
Section 2: CKN’s inequality for fractional Sobolev spaces
SLIDE 16 CKN’s inequality for fractional Sobolev spaces
- Goals: extending CKN’s inequality for fractional Sobolev spaces
and searching for variants of Hardy’s inequality when p > d. Recall
|u|p
Ws,p :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|p |x − y|d+sp dx dy for u ∈ Lp(Rd).
- Known results: (Hardy’s type-inequalities):
Mazya & Shaposhnikova JFA 02 (harmonic analysis, extension technique), Frank & Seiringer JFA 08 (ground state representation formula): a = 1, τ = p, α = 0 and γ = −s. Abdellaoui & Bentifour JFA 17 (Picone’s inequality): a = 1,
τ = pd/(d − sp), −(d − sp)/p < α = γ < 0, and 1 < p < d/s.
Sharp constant and the remainder are considered by Frank & Seiringer and Abdellaoui & Bentifour.
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 17 CKN’s inequality for fractional Sobolev spaces
- Goals: extending CKN’s inequality for fractional Sobolev spaces
and searching for variants of Hardy’s inequality when p > d. Recall
|u|p
Ws,p :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|p |x − y|d+sp dx dy for u ∈ Lp(Rd).
- Known results: (Hardy’s type-inequalities):
Mazya & Shaposhnikova JFA 02 (harmonic analysis, extension technique), Frank & Seiringer JFA 08 (ground state representation formula): a = 1, τ = p, α = 0 and γ = −s. Abdellaoui & Bentifour JFA 17 (Picone’s inequality): a = 1,
τ = pd/(d − sp), −(d − sp)/p < α = γ < 0, and 1 < p < d/s.
Sharp constant and the remainder are considered by Frank & Seiringer and Abdellaoui & Bentifour.
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 18 CKN’s inequality for fractional Sobolev spaces
- Goals: extending CKN’s inequality for fractional Sobolev spaces
and searching for variants of Hardy’s inequality when p > d. Recall
|u|p
Ws,p :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|p |x − y|d+sp dx dy for u ∈ Lp(Rd).
- Known results: (Hardy’s type-inequalities):
Mazya & Shaposhnikova JFA 02 (harmonic analysis, extension technique), Frank & Seiringer JFA 08 (ground state representation formula): a = 1, τ = p, α = 0 and γ = −s. Abdellaoui & Bentifour JFA 17 (Picone’s inequality): a = 1,
τ = pd/(d − sp), −(d − sp)/p < α = γ < 0, and 1 < p < d/s.
Sharp constant and the remainder are considered by Frank & Seiringer and Abdellaoui & Bentifour.
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 19 CKN’s inequality for fractional Sobolev spaces
- Goals: extending CKN’s inequality for fractional Sobolev spaces
and searching for variants of Hardy’s inequality when p > d. Recall
|u|p
Ws,p :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|p |x − y|d+sp dx dy for u ∈ Lp(Rd).
- Known results: (Hardy’s type-inequalities):
Mazya & Shaposhnikova JFA 02 (harmonic analysis, extension technique), Frank & Seiringer JFA 08 (ground state representation formula): a = 1, τ = p, α = 0 and γ = −s. Abdellaoui & Bentifour JFA 17 (Picone’s inequality): a = 1,
τ = pd/(d − sp), −(d − sp)/p < α = γ < 0, and 1 < p < d/s.
Sharp constant and the remainder are considered by Frank & Seiringer and Abdellaoui & Bentifour.
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 20 CKN’s inequality for fractional Sobolev spaces
- Goals: extending CKN’s inequality for fractional Sobolev spaces
and searching for variants of Hardy’s inequality when p > d. Recall
|u|p
Ws,p :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|p |x − y|d+sp dx dy for u ∈ Lp(Rd).
- Known results: (Hardy’s type-inequalities):
Mazya & Shaposhnikova JFA 02 (harmonic analysis, extension technique), Frank & Seiringer JFA 08 (ground state representation formula): a = 1, τ = p, α = 0 and γ = −s. Abdellaoui & Bentifour JFA 17 (Picone’s inequality): a = 1,
τ = pd/(d − sp), −(d − sp)/p < α = γ < 0, and 1 < p < d/s.
Sharp constant and the remainder are considered by Frank & Seiringer and Abdellaoui & Bentifour.
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 21 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 22 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 23 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 24 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 25 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 26 Statement of the results
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.1) and, with γ = aσ + (1 − a)β, 0 α − σ and
τ + γ d = 1 p + α − s d
(2.2) Theorem (Ng. & Squassina JFA 17) Assume (2.1) and (2.2). If 1/τ + γ/d > 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
and if 1/τ + γ/d < 0 then
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd \ {0}).
SLIDE 27
Our approach
Starting point: Sobolev’s and Poincare’s inequalities; NO integration by parts. Inspiration: harmonic analysis; however, instead of localizing frequency, we localize space variables. The interpolation part is inspired from the proof of CKN’s inequality.
SLIDE 28
Our approach
Starting point: Sobolev’s and Poincare’s inequalities; NO integration by parts. Inspiration: harmonic analysis; however, instead of localizing frequency, we localize space variables. The interpolation part is inspired from the proof of CKN’s inequality.
SLIDE 29
Our approach
Starting point: Sobolev’s and Poincare’s inequalities; NO integration by parts. Inspiration: harmonic analysis; however, instead of localizing frequency, we localize space variables. The interpolation part is inspired from the proof of CKN’s inequality.
SLIDE 30
Our approach
Starting point: Sobolev’s and Poincare’s inequalities; NO integration by parts. Inspiration: harmonic analysis; however, instead of localizing frequency, we localize space variables. The interpolation part is inspired from the proof of CKN’s inequality.
SLIDE 31 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 32 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 33 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 34 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 35 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 36 A new proof of Hardy’s inequality
Recall Hardy’s inequality, for 1 p < d, ˆ
Rd
|u|p |x|p dx C
ˆ
Rd |∇u|p dx
for u ∈ C1
c(Rd).
Here is the proof. Set
Ck :=
By Poincare’s inequality, we have
Ck
Ck
u
dx C2kp
Ck
|∇u|p dx,
which yields ˆ
Ck
|u|p |x|p dx ∼ 2−kp
ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C2k(d−p)
u
. By Poincare’s inequality, we also have
u −
Ck
u
dx C2kp
Ck∪Ck+1
|∇u|p dx.
SLIDE 37 It follows that 2k(d−p)
u
Cc
ˆ
Ck∪Ck+1
|∇u|p dx+c2(k+1)(d−p)
u
. for c > 2p−d, in particular for c = (2p−d + 1)/2 < 1. This implies
2k(d−p)
u
C
ˆ
Ck∪Ck+1
|∇u|p dx C
ˆ
Rd |∇u|p.
We derive that
2−kp ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C
2k(d−p)
u
C
ˆ
Rd |∇u|p.
The proof is complete.
SLIDE 38 It follows that 2k(d−p)
u
Cc
ˆ
Ck∪Ck+1
|∇u|p dx+c2(k+1)(d−p)
u
. for c > 2p−d, in particular for c = (2p−d + 1)/2 < 1. This implies
2k(d−p)
u
C
ˆ
Ck∪Ck+1
|∇u|p dx C
ˆ
Rd |∇u|p.
We derive that
2−kp ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C
2k(d−p)
u
C
ˆ
Rd |∇u|p.
The proof is complete.
SLIDE 39 It follows that 2k(d−p)
u
Cc
ˆ
Ck∪Ck+1
|∇u|p dx+c2(k+1)(d−p)
u
. for c > 2p−d, in particular for c = (2p−d + 1)/2 < 1. This implies
2k(d−p)
u
C
ˆ
Ck∪Ck+1
|∇u|p dx C
ˆ
Rd |∇u|p.
We derive that
2−kp ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C
2k(d−p)
u
C
ˆ
Rd |∇u|p.
The proof is complete.
SLIDE 40 It follows that 2k(d−p)
u
Cc
ˆ
Ck∪Ck+1
|∇u|p dx+c2(k+1)(d−p)
u
. for c > 2p−d, in particular for c = (2p−d + 1)/2 < 1. This implies
2k(d−p)
u
C
ˆ
Ck∪Ck+1
|∇u|p dx C
ˆ
Rd |∇u|p.
We derive that
2−kp ˆ
Ck
|u|p C
ˆ
Ck
|∇u|p dx + C
2k(d−p)
u
C
ˆ
Rd |∇u|p.
The proof is complete.
SLIDE 41 Proof of CKN’s inequality for the main case
Let p > 1, q 1, τ > 0, 0 < s < 1, 0 < a 1, α, β, γ ∈ R be s.t. 1
τ + γ d = a 1 p + α − s d
1 q + β d
(2.3) and, with γ = aσ + (1 − a)β, 0 α − σ s (2.4) Theorem Assume (2.3) and (2.4). We have, for 1/τ + γ/d > 0,
|x|γuLτ(Rd) C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd)
∀ u ∈ C1
c(Rd),
|u|p
Ws,p,α(Rd) =
ˆ
Rd
ˆ
Rd
|x|
αp 2 |y| αp 2 |u(x) − u(y)|p
|x − y|d+sp dx dy.
SLIDE 42 Lemma (Gagliardo-Nirenberg’s inequality) Let d 1, 0 < s < 1, p > 1, q 1, τ > 0, and 0 < a 1 be s.t. 1
τ = a 1 p − s d
q.
We have
uLτ(Rd) C|u|a
Ws,p(Rd)u1−a Lq(Rd)
for u ∈ C1
c(Rd).
SLIDE 43 Lemma (Gagliardo-Nirenberg’s inequality) Let d 1, 0 < s < 1, p > 1, q 1, τ > 0, and 0 < a 1 be s.t. 1
τ = a 1 p − s d
q.
We have
uLτ(Rd) C|u|a
Ws,p(Rd)u1−a Lq(Rd)
for u ∈ C1
c(Rd).
SLIDE 44 Lemma Let d 1, p > 1, 0 < s < 1, q 1, τ > 0, and 0 < a 1 be s.t. 1
τ a 1 p − s d
q.
Let λ > 0, 0 < r < R, and set D :=
. Then, ∀u ∈ C1(¯ D),
D
u
dx 1/τ C
Ws,p(D)
a/p
D
|u|q dx (1−a)/q
.
SLIDE 45 Lemma Let d 1, p > 1, 0 < s < 1, q 1, τ > 0, and 0 < a 1 be s.t. 1
τ a 1 p − s d
q.
Let λ > 0, 0 < r < R, and set D :=
. Then, ∀u ∈ C1(¯ D),
D
u
dx 1/τ C
Ws,p(D)
a/p
D
|u|q dx (1−a)/q
.
SLIDE 46 Lemma Let d 1, p > 1, 0 < s < 1, q 1, τ > 0, and 0 < a 1 be s.t. 1
τ a 1 p − s d
q.
Let λ > 0, 0 < r < R, and set D :=
. Then, ∀u ∈ C1(¯ D),
D
u
dx 1/τ C
Ws,p(D)
a/p
D
|u|q dx (1−a)/q
.
SLIDE 47
- Proof. By scaling, one can assume that λ = 1. Let 0 < s′ s and
τ′ τ be such that
1
τ′ = a 1 p − s′ d
q.
From the previous lemma, we derive that
D
u
C |u|a
Ws′,p(D) u1−a Lq(D).
Since |u|Ws′,p(D) C |u|Ws,p(D), uLτ(D) CuLτ′(D), the conclusion follows.
SLIDE 48
- Proof. By scaling, one can assume that λ = 1. Let 0 < s′ s and
τ′ τ be such that
1
τ′ = a 1 p − s′ d
q.
From the previous lemma, we derive that
D
u
C |u|a
Ws′,p(D) u1−a Lq(D).
Since |u|Ws′,p(D) C |u|Ws,p(D), uLτ(D) CuLτ′(D), the conclusion follows.
SLIDE 49
- Proof. By scaling, one can assume that λ = 1. Let 0 < s′ s and
τ′ τ be such that
1
τ′ = a 1 p − s′ d
q.
From the previous lemma, we derive that
D
u
C |u|a
Ws′,p(D) u1−a Lq(D).
Since |u|Ws′,p(D) C |u|Ws,p(D), uLτ(D) CuLτ′(D), the conclusion follows.
SLIDE 50
- Proof. By scaling, one can assume that λ = 1. Let 0 < s′ s and
τ′ τ be such that
1
τ′ = a 1 p − s′ d
q.
From the previous lemma, we derive that
D
u
C |u|a
Ws′,p(D) u1−a Lq(D).
Since |u|Ws′,p(D) C |u|Ws,p(D), uLτ(D) CuLτ′(D), the conclusion follows.
SLIDE 51 Proof of CKN’s inequality
Recall Ck :=
- x ∈ Rd : 2k |x| < 2k+1. We have,
- α − σ 0 +
balance law
1
τ a 1 p − s d
q.
It follows that
Ck
u
dx 1/τ C
Ws,p(Ck)
a/p
Ck
|u|q dx (1−a)/q
. Using the balance law, we derive that ˆ
Ck
|x|γτ|u|τ dx C|u|aτ
Ws,p,α(Ck)|x|βu(1−a)τ Lq(Ck) +C2(γτ+d)k
u
, (2.5)
SLIDE 52 Proof of CKN’s inequality
Recall Ck :=
- x ∈ Rd : 2k |x| < 2k+1. We have,
- α − σ 0 +
balance law
1
τ a 1 p − s d
q.
It follows that
Ck
u
dx 1/τ C
Ws,p(Ck)
a/p
Ck
|u|q dx (1−a)/q
. Using the balance law, we derive that ˆ
Ck
|x|γτ|u|τ dx C|u|aτ
Ws,p,α(Ck)|x|βu(1−a)τ Lq(Ck) +C2(γτ+d)k
u
, (2.5)
SLIDE 53 Proof of CKN’s inequality
Recall Ck :=
- x ∈ Rd : 2k |x| < 2k+1. We have,
- α − σ 0 +
balance law
1
τ a 1 p − s d
q.
It follows that
Ck
u
dx 1/τ C
Ws,p(Ck)
a/p
Ck
|u|q dx (1−a)/q
. Using the balance law, we derive that ˆ
Ck
|x|γτ|u|τ dx C|u|aτ
Ws,p,α(Ck)|x|βu(1−a)τ Lq(Ck) +C2(γτ+d)k
u
, (2.5)
SLIDE 54 Proof of CKN’s inequality
Recall Ck :=
- x ∈ Rd : 2k |x| < 2k+1. We have,
- α − σ 0 +
balance law
1
τ a 1 p − s d
q.
It follows that
Ck
u
dx 1/τ C
Ws,p(Ck)
a/p
Ck
|u|q dx (1−a)/q
. Using the balance law, we derive that ˆ
Ck
|x|γτ|u|τ dx C|u|aτ
Ws,p,α(Ck)|x|βu(1−a)τ Lq(Ck) +C2(γτ+d)k
u
, (2.5)
SLIDE 55 Since
u −
Ck+1
u
C
Ws,p(Ck∪Ck+1)
aτ/p
Ck∪Ck+1
|u|q dx (1−a)τ/q
, we obtain, with c = 2/(1 + 2γτ+d) < 1, 2(γτ+d)k
u
C|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1)
+ c2(γτ+d)(k+1)
u
. This yields
2(γτ+d)k
u
C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
(2.6)
SLIDE 56 Since
u −
Ck+1
u
C
Ws,p(Ck∪Ck+1)
aτ/p
Ck∪Ck+1
|u|q dx (1−a)τ/q
, we obtain, with c = 2/(1 + 2γτ+d) < 1, 2(γτ+d)k
u
C|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1)
+ c2(γτ+d)(k+1)
u
. This yields
2(γτ+d)k
u
C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
(2.6)
SLIDE 57 Combining (2.5) and (2.6) yields ˆ
Rd |x|γτ|u|τ dx C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
One has, for s 0, t 0 with s + t 1, and for xk 0 and
yk 0,
n
xs
kyt k
xk s
n
yk t
. Applying this inequality with s = aτ/p and t = (1 − a)τ/q, we
ˆ
Rd |x|γτ|u|τ dx C|u|aτ Ws,p,α(∞
k=m Ck)|x|βu(1−a)τ
Lq(∞
k=m Ck),
since a/p + (1 − a)/q 1/τ thanks to the fact α − σ s.
SLIDE 58 Combining (2.5) and (2.6) yields ˆ
Rd |x|γτ|u|τ dx C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
One has, for s 0, t 0 with s + t 1, and for xk 0 and
yk 0,
n
xs
kyt k
xk s
n
yk t
. Applying this inequality with s = aτ/p and t = (1 − a)τ/q, we
ˆ
Rd |x|γτ|u|τ dx C|u|aτ Ws,p,α(∞
k=m Ck)|x|βu(1−a)τ
Lq(∞
k=m Ck),
since a/p + (1 − a)/q 1/τ thanks to the fact α − σ s.
SLIDE 59 Combining (2.5) and (2.6) yields ˆ
Rd |x|γτ|u|τ dx C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
One has, for s 0, t 0 with s + t 1, and for xk 0 and
yk 0,
n
xs
kyt k
xk s
n
yk t
. Applying this inequality with s = aτ/p and t = (1 − a)τ/q, we
ˆ
Rd |x|γτ|u|τ dx C|u|aτ Ws,p,α(∞
k=m Ck)|x|βu(1−a)τ
Lq(∞
k=m Ck),
since a/p + (1 − a)/q 1/τ thanks to the fact α − σ s.
SLIDE 60 Combining (2.5) and (2.6) yields ˆ
Rd |x|γτ|u|τ dx C
|u|aτ
Ws,p,α(Ck∪Ck+1)|x|βu(1−a)τ Lq(Ck∪Ck+1).
One has, for s 0, t 0 with s + t 1, and for xk 0 and
yk 0,
n
xs
kyt k
xk s
n
yk t
. Applying this inequality with s = aτ/p and t = (1 − a)τ/q, we
ˆ
Rd |x|γτ|u|τ dx C|u|aτ Ws,p,α(∞
k=m Ck)|x|βu(1−a)τ
Lq(∞
k=m Ck),
since a/p + (1 − a)/q 1/τ thanks to the fact α − σ s.
SLIDE 61 On the limiting case
Theorem (Ng. & Squassina JFA 17) Let d 1, p > 1, 0 < s < 1, q 1, τ > 1, 0 < a 1, α, β, γ ∈ R be such that (2.3) holds and 0 a − σ s. Let u ∈ C1
c(Rd), and 0 < r < R. We have
i) if 1/τ + γ/d = 0 and supp u ⊂ BR, then
ˆ
Rd
|x|γτ
lnτ(2R/|x|)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd),
ii) if 1/τ + γ/d = 0 and supp u ∩ Br = ∅, then
ˆ
Rd
|x|γτ
lnτ(2|x|/r)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd).
SLIDE 62 On the limiting case
Theorem (Ng. & Squassina JFA 17) Let d 1, p > 1, 0 < s < 1, q 1, τ > 1, 0 < a 1, α, β, γ ∈ R be such that (2.3) holds and 0 a − σ s. Let u ∈ C1
c(Rd), and 0 < r < R. We have
i) if 1/τ + γ/d = 0 and supp u ⊂ BR, then
ˆ
Rd
|x|γτ
lnτ(2R/|x|)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd),
ii) if 1/τ + γ/d = 0 and supp u ∩ Br = ∅, then
ˆ
Rd
|x|γτ
lnτ(2|x|/r)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd).
SLIDE 63 On the limiting case
Theorem (Ng. & Squassina JFA 17) Let d 1, p > 1, 0 < s < 1, q 1, τ > 1, 0 < a 1, α, β, γ ∈ R be such that (2.3) holds and 0 a − σ s. Let u ∈ C1
c(Rd), and 0 < r < R. We have
i) if 1/τ + γ/d = 0 and supp u ⊂ BR, then
ˆ
Rd
|x|γτ
lnτ(2R/|x|)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd),
ii) if 1/τ + γ/d = 0 and supp u ∩ Br = ∅, then
ˆ
Rd
|x|γτ
lnτ(2|x|/r)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd).
SLIDE 64 On the limiting case
Theorem (Ng. & Squassina JFA 17) Let d 1, p > 1, 0 < s < 1, q 1, τ > 1, 0 < a 1, α, β, γ ∈ R be such that (2.3) holds and 0 a − σ s. Let u ∈ C1
c(Rd), and 0 < r < R. We have
i) if 1/τ + γ/d = 0 and supp u ⊂ BR, then
ˆ
Rd
|x|γτ
lnτ(2R/|x|)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd),
ii) if 1/τ + γ/d = 0 and supp u ∩ Br = ∅, then
ˆ
Rd
|x|γτ
lnτ(2|x|/r)|u|τ dx
1/τ C|u|a
Ws,p,α(Rd)|x|βu(1−a) Lq(Rd).
SLIDE 65
Section 3: New perspectives of Hardy’s and Caffarelli, Kohn, Nirenberg’s inequalities
SLIDE 66 Motivations
Define, for d 1 and p 1,
Iδ(u) :=
ˆ
Rd
ˆ
Rd |u(x)−u(y)|>δ
δp |x − y|d+p dx dy ∀ u ∈ Lp(Rd).
1 Iδ is related to the semi-norm of Ws,q(Rd):
|u|q
Ws,q(Rd) :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|q |x − y|d+sq dx dy.
2 Iδ appears in an estimate for the topological degree due to
Bourgain, Brezis, & Ng., CRAS 05, and Ng. JAM 07
| deg u| Cd
ˆ
Sd
ˆ
Sd |u(x)−u(y)|ℓd
1
|x − y|2d dx dy, ∀ u ∈ C(Sd, Sd),
where ℓd =
2 d+1.
SLIDE 67 Motivations
Define, for d 1 and p 1,
Iδ(u) :=
ˆ
Rd
ˆ
Rd |u(x)−u(y)|>δ
δp |x − y|d+p dx dy ∀ u ∈ Lp(Rd).
1 Iδ is related to the semi-norm of Ws,q(Rd):
|u|q
Ws,q(Rd) :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|q |x − y|d+sq dx dy.
2 Iδ appears in an estimate for the topological degree due to
Bourgain, Brezis, & Ng., CRAS 05, and Ng. JAM 07
| deg u| Cd
ˆ
Sd
ˆ
Sd |u(x)−u(y)|ℓd
1
|x − y|2d dx dy, ∀ u ∈ C(Sd, Sd),
where ℓd =
2 d+1.
SLIDE 68 Motivations
Define, for d 1 and p 1,
Iδ(u) :=
ˆ
Rd
ˆ
Rd |u(x)−u(y)|>δ
δp |x − y|d+p dx dy ∀ u ∈ Lp(Rd).
1 Iδ is related to the semi-norm of Ws,q(Rd):
|u|q
Ws,q(Rd) :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|q |x − y|d+sq dx dy.
2 Iδ appears in an estimate for the topological degree due to
Bourgain, Brezis, & Ng., CRAS 05, and Ng. JAM 07
| deg u| Cd
ˆ
Sd
ˆ
Sd |u(x)−u(y)|ℓd
1
|x − y|2d dx dy, ∀ u ∈ C(Sd, Sd),
where ℓd =
2 d+1.
SLIDE 69 Motivations
Define, for d 1 and p 1,
Iδ(u) :=
ˆ
Rd
ˆ
Rd |u(x)−u(y)|>δ
δp |x − y|d+p dx dy ∀ u ∈ Lp(Rd).
1 Iδ is related to the semi-norm of Ws,q(Rd):
|u|q
Ws,q(Rd) :=
ˆ
Rd
ˆ
Rd
|u(x) − u(y)|q |x − y|d+sq dx dy.
2 Iδ appears in an estimate for the topological degree due to
Bourgain, Brezis, & Ng., CRAS 05, and Ng. JAM 07
| deg u| Cd
ˆ
Sd
ˆ
Sd |u(x)−u(y)|ℓd
1
|x − y|2d dx dy, ∀ u ∈ C(Sd, Sd),
where ℓd =
2 d+1.
SLIDE 70 Theorem (Ng. JFA 06, Bourgain & Ng. CRAS 06) Let d 1, 1 < p < +∞ and u ∈ Lp(Rd). Then
1
Iδ(u) Cd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
2
lim
δ→0 Iδ(u) = Kd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
3 If
lim inf
δ→0 Iδ(u) < +∞,
then u ∈ W1,p(Rd). Related works: Bourgain, Brezis, & Mironescu 01, Davila 02.
SLIDE 71 Theorem (Ng. JFA 06, Bourgain & Ng. CRAS 06) Let d 1, 1 < p < +∞ and u ∈ Lp(Rd). Then
1
Iδ(u) Cd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
2
lim
δ→0 Iδ(u) = Kd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
3 If
lim inf
δ→0 Iδ(u) < +∞,
then u ∈ W1,p(Rd). Related works: Bourgain, Brezis, & Mironescu 01, Davila 02.
SLIDE 72 Theorem (Ng. JFA 06, Bourgain & Ng. CRAS 06) Let d 1, 1 < p < +∞ and u ∈ Lp(Rd). Then
1
Iδ(u) Cd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
2
lim
δ→0 Iδ(u) = Kd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
3 If
lim inf
δ→0 Iδ(u) < +∞,
then u ∈ W1,p(Rd). Related works: Bourgain, Brezis, & Mironescu 01, Davila 02.
SLIDE 73 Theorem (Ng. JFA 06, Bourgain & Ng. CRAS 06) Let d 1, 1 < p < +∞ and u ∈ Lp(Rd). Then
1
Iδ(u) Cd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
2
lim
δ→0 Iδ(u) = Kd,p
ˆ
Rd |∇u|p
∀ u ∈ W1,p(Rd).
3 If
lim inf
δ→0 Iδ(u) < +∞,
then u ∈ W1,p(Rd). Related works: Bourgain, Brezis, & Mironescu 01, Davila 02.
SLIDE 74 Theorem (Ng. CVPDE, 11) Let p 1, Q be a cube or a ball of Rd. Then ∃C > 0 s.t. for all
δ > 0:
¨
Q2 |u(x) − u(y)|p dx dy
C
d+p d
¨
Q2 |u(x)−u(y)|>δ
δp |x − y|d+p dx dy + δp|Q|2
. A variant of Sobolev’s inequality also holds for Iδ for 1 < p < d.
Question: How’s about Hardy’s and Caffarelli, Kohn, Nirenberg’s inequalities?
SLIDE 75 Variants of Hardy’s inequalities
Theorem (Ng. & Squassina JAM, to appear) Let d 1, p 1, 0 < r < R, and u ∈ Lp(Rd). We have i) if 1 p < d and supp u ⊂ BR, then ˆ
Rd
|u(x)|p |x|p dx C
ii) if p > d and supp u ⊂ Rd \ Br, then ˆ
Rd
|u(x)|p |x|p dx C
Similar results hold for the case p = d.
SLIDE 76 Variants of Hardy’s inequalities
Theorem (Ng. & Squassina JAM, to appear) Let d 1, p 1, 0 < r < R, and u ∈ Lp(Rd). We have i) if 1 p < d and supp u ⊂ BR, then ˆ
Rd
|u(x)|p |x|p dx C
ii) if p > d and supp u ⊂ Rd \ Br, then ˆ
Rd
|u(x)|p |x|p dx C
Similar results hold for the case p = d.
SLIDE 77 Variants of Hardy’s inequalities
Theorem (Ng. & Squassina JAM, to appear) Let d 1, p 1, 0 < r < R, and u ∈ Lp(Rd). We have i) if 1 p < d and supp u ⊂ BR, then ˆ
Rd
|u(x)|p |x|p dx C
ii) if p > d and supp u ⊂ Rd \ Br, then ˆ
Rd
|u(x)|p |x|p dx C
Similar results hold for the case p = d.
SLIDE 78 Theorem (Ng. & Squassina JAM, to appear) Let d 2, 1 < p < d, τ > 0, 0 < r < R, and u ∈ Lp
loc(Rd). Assume
that 1
τ + γ d = 1 p + α − 1 d
and 0 α − γ 1. We have i) if d − p + pα > 0 and supp u ⊂ BR, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
ii) if d − p + pα < 0 and supp u ⊂ Rd \ Br, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
- Iδ(u, α) + rd−p+pαδp.
- Variants for p = d 2 and also for p = d = 1 hold.
- Variants for 0 < a < 1 hold.
SLIDE 79 Theorem (Ng. & Squassina JAM, to appear) Let d 2, 1 < p < d, τ > 0, 0 < r < R, and u ∈ Lp
loc(Rd). Assume
that 1
τ + γ d = 1 p + α − 1 d
and 0 α − γ 1. We have i) if d − p + pα > 0 and supp u ⊂ BR, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
ii) if d − p + pα < 0 and supp u ⊂ Rd \ Br, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
- Iδ(u, α) + rd−p+pαδp.
- Variants for p = d 2 and also for p = d = 1 hold.
- Variants for 0 < a < 1 hold.
SLIDE 80 Theorem (Ng. & Squassina JAM, to appear) Let d 2, 1 < p < d, τ > 0, 0 < r < R, and u ∈ Lp
loc(Rd). Assume
that 1
τ + γ d = 1 p + α − 1 d
and 0 α − γ 1. We have i) if d − p + pα > 0 and supp u ⊂ BR, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
ii) if d − p + pα < 0 and supp u ⊂ Rd \ Br, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
- Iδ(u, α) + rd−p+pαδp.
- Variants for p = d 2 and also for p = d = 1 hold.
- Variants for 0 < a < 1 hold.
SLIDE 81 Theorem (Ng. & Squassina JAM, to appear) Let d 2, 1 < p < d, τ > 0, 0 < r < R, and u ∈ Lp
loc(Rd). Assume
that 1
τ + γ d = 1 p + α − 1 d
and 0 α − γ 1. We have i) if d − p + pα > 0 and supp u ⊂ BR, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
ii) if d − p + pα < 0 and supp u ⊂ Rd \ Br, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
- Iδ(u, α) + rd−p+pαδp.
- Variants for p = d 2 and also for p = d = 1 hold.
- Variants for 0 < a < 1 hold.
SLIDE 82 Theorem (Ng. & Squassina JAM, to appear) Let d 2, 1 < p < d, τ > 0, 0 < r < R, and u ∈ Lp
loc(Rd). Assume
that 1
τ + γ d = 1 p + α − 1 d
and 0 α − γ 1. We have i) if d − p + pα > 0 and supp u ⊂ BR, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
ii) if d − p + pα < 0 and supp u ⊂ Rd \ Br, then
ˆ
Rd |x|γτ|u(x)|τ dx
p/τ C
- Iδ(u, α) + rd−p+pαδp.
- Variants for p = d 2 and also for p = d = 1 hold.
- Variants for 0 < a < 1 hold.
SLIDE 83
Thank you for your attention!