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diffusions

Jean Dolbeault

http://www.ceremade.dauphine.fr/ ∼ dolbeaul Ceremade, Universit´e Paris-Dauphine

July 7, 2015

CMO Workshop 15w5049 on Kinetic and Related Equations,

Oaxaca, July 6-10, 2015

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Introduction

1

Caffarelli-Kohn-Nirenberg inequalities

2

Entropy and the fast diffusion equation

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Caffarelli-Kohn-Nirenberg inequalities

The symmetry issue —

In collaboration with M.J. Esteban and M. Loss

⊲ Nonlinear flows (fast diffusion equation) can be used as a tool for the investigation of sharp functional inequalities

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Caffarelli-Kohn-Nirenberg inequalities and the symmetry breaking issue

Let D a,b := n

v ∈ L p R d , | x | −b dx

: | x | −a |∇ v | ∈ L 2 R d , dx o Z

R

d

| v | p

| x | b p dx 2/p

≤ C a,b

Z

R

d

|∇ v | 2

| x | 2 a dx ∀ v ∈ D a,b

hold under the conditions that a ≤ b ≤ a + 1 if d ≥ 3, a < b ≤ a + 1 if d = 2, a + 1/2 < b ≤ a + 1 if d = 1, and a < a c := (d − 2)/2

p = 2 d

d − 2 + 2 (b − a)

⊲ With v ⋆ (x ) =

1 + | x | (p 2) (a

c

a)

p−22

and C a,b = k | x | −b v ⋆ k 2 p

k | x | a ∇ v ⋆ k 2 2

do we have C a,b = C a,b (symmetry)

or C a,b > C a,b (symmetry breaking) ?

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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CKN: range of the parameters

Figure: d = 3 Z

R

d

| v | p

| x | b p dx 2/p

≤ C a,b

Z

R

d

|∇ v | 2

| x | 2 a dx

a ≤ b ≤ a + 1 if d ≥ 3

a < b ≤ a + 1 if d = 2, a + 1/2 < b ≤ a + 1 if d = 1 and a < a c := (d − 2)/2

p = 2 d

d − 2 + 2 (b − a)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Symmetry vs. symmetry breaking

[J.D., Esteban, Loss, Tarantello, 2009] There is a curve which separates the symmetry region from the symmetry breaking region, which is parametrized by a function p 7→ a + b

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Moving planes and symmetrization techniques

[Chou, Chu], [Horiuchi]

[Betta, Brock, Marcaldo, Posteraro]

+ Perturbation results: [CS Lin, ZQ Wang], [Smets, Willem], [JD, Esteban, Tarantello 2007], [J.D., Esteban, Loss, Tarantello, 2009]

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Linear instability of radial minimizers:

the Felli-Schneider curve

[Catrina, Wang], [Felli, Schneider] The functional C a,b

Z

R

d

|∇ v | 2

| x | 2 a dx − Z

R

d

| v | p

| x | b p dx 2/p

is linearly instable at v = v ⋆

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Direct spectral estimates

[J.D., Esteban, Loss, 2011]: sharp interpolation on the sphere and a Keller-Lieb-Thirring spectral estimate on the line

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Numerical results

20 40 60 80 100

10 20 30 40 50

Λ(µ) symmetric non-symmetric asymptotic

bifurcation µ α

Parametric plot of the branch of optimal functions for p = 2.8, d = 5.

Non-symmetric solutions bifurcate from symmetric ones at a bifurcation point computed by V. Felli and M. Schneider. The branch behaves for large values of Λ as predicted by F. Catrina and Z.-Q. Wang

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Other evidences

Further numerical results [J.D., Esteban, 2012]

Formal commutation of the non-symmetric branch near the bifurcation point [J.D., Esteban, 2013]

Asymptotic energy estimates [J.D., Esteban, 2013]

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Symmetry vs. symmetry breaking:

the sharp result

A result based on entropies and nonlinear flows

[J.D., Esteban, Loss, 2015]: http://arxiv.org/abs/1506.03664

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The symmetry result

The Felli & Schneider curve is defined by b FS (a) := d (a c − a)

2 p

(a c − a) 2 + d − 1 + a − a c

Theorem

Let d ≥ 2 and p < 2 . If either a ∈ [0, a c ) and b > 0, or a < 0 and b ≥ b FS (a), then the optimal functions for the Caffarelli-Kohn-Nirenberg inequalities are radially symmetric

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The Emden-Fowler transformation and the cylinder

⊲ With an Emden-Fowler transformation, Caffarelli-Kohn-Nirenberg inequalities on the Euclidean space are equivalent to

Gagliardo-Nirenberg inequalities on a cylinder

v (r , ω) = r a a

c

ϕ(s, ω) with r = | x | , s = − log r and ω = x r With this transformation, the Caffarelli-Kohn-Nirenberg inequalities can be rewritten as

k ∂ s ϕ k 2 L

2

( C ) + k∇ ω ϕ k 2 L

2

( C ) + Λ k ϕ k 2 L

2

( C ) ≥ µ(Λ) k ϕ k 2 L

p

( C ) ∀ ϕ ∈ H 1 ( C )

where Λ := (a c − a) 2 , C = R × S d− 1 and the optimal constant µ(Λ) is µ(Λ) = 1

C a,b

with a = a c ± √

Λ and b = d p ± √

Λ

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Entropy and the fast diffusion equation (2000-2014)

A short review —

⊲ Relative entropy, linearization, functional inequalities, improvements, improved rates of convergence, delays

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The fast diffusion equation

The fast diffusion equation corresponds to m < 1 u t = ∆u m x ∈ R d , t > 0

Self-similar (Barenblatt) function: U (t) = O(t d/(2 d(1 m)) ) as t → + ∞

[Friedmann, Kamin, 1980] k u(t, · ) − U (t, · ) k L

= o(t d/(2 d(1 m)) )

⊲ Entropy methods allow to measure the speed of convergence of any solution to U in norms which are adapted to the equation

⊲ Entropy methods provide explicit constants

The Bakry-Emery method [Carrillo, Toscani], [Juengel, Markowich, Toscani], [Carrillo, Juengel, Markowich, Toscani, Unterreiter], [Carrillo, V´ azquez]

The variational approach and Gagliardo-Nirenberg inequalities:

[del Pino, JD]

Mass transportation and gradient flow issues: [Otto et al.]

Large time asymptotics and the spectral approach: [Blanchet, Bonforte, JD, Grillo, V´ azquez]

Refined relative entropy methods

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Time-dependent rescaling, free energy

Time-dependent rescaling: Take u(τ, y ) = R −d (τ) v (t , y /R(τ)) where

dR

dτ = R d(1 −m) 1 , R(0) = 1 , t = log R The function v solves a Fokker-Planck type equation

∂v

∂t = ∆v m + ∇ · (x v) , v | τ=0 = u 0

[Ralston, Newman, 1984] Lyapunov functional:

Generalized entropy or Free energy F [v ] :=

Z

R

d

v m m − 1 + 1

2 | x | 2 v

dx − F 0

Entropy production is measured by the Generalized Fisher information

d

dt F [v ] = −I [v ] , I [v ] :=

Z

R

d

v

∇ v m v + x

2

dx

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Relative entropy and entropy production

Stationary solution: choose C such that k v k L

1

= k u k L

1

= M > 0 v (x ) := C + 1 2m −m | x | 2 − 1/(1 −m)

+

Relative entropy: Fix F 0 so that F [v ] = 0 Entropy – entropy production inequality

Theorem

d ≥ 3, m ∈ [ d d 1 , + ∞ ), m > 1 2 , m 6 = 1 I [v] ≥ 2 F [v ]

Corollary

A solution v with initial data u 0 ∈ L 1 + ( R d ) such that | x | 2 u 0 ∈ L 1 ( R d ), u 0 m ∈ L 1 ( R d ) satisfies F [v(t , · )] ≤ F [u 0 ] e 2 t

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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An equivalent formulation: Gagliardo-Nirenberg inequalities

F [v] = Z

R

d

v m m − 1 + 1

2 | x | 2 v

dx −F 0 ≤ 1 2 Z

R

d

v

∇ v m v + x

2

dx = 1 2 I [v]

Rewrite it with p = 2m− 1 1 , v = w 2p , v m = w p+1 as 1

2 2m

2m − 1 2 Z

R

d

|∇ w | 2 dx + 1

1 − m − d Z

R

d

| w | 1+p dx − K ≥ 0 for some γ, K = K 0

R

R

d

v dx = R

R

d

w 2p dx γ

w = w = v 1/2p is optimal Theorem

[Del Pino, J.D.] With 1 < p ≤ d d 2 (fast diffusion case) and d ≥ 3 k w k L

2p

( R

d

) ≤ C p,d GN k∇ w k θ L

2

( R

d

) k w k 1 L

p+1

θ ( R

d

)

C p,d GN =

y(p− 1)

2

2πd

θ2

2y − d 2y

2p1

Γ(y)

Γ(y −

d2

)

θd

, θ = p(d+2 d(p− (d 1) 2)p) , y = p+1 p 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Entropy methods and linearization: sharp asymptotic rates of convergence

Generalized Barenblatt profiles: V D (x) := D + | x | 2

m−11

(H1) V D

0

≤ v 0 ≤ V D

1

for some D 0 > D 1 > 0

(H2) if d ≥ 3 and m ≤ m := d− d− 4 2 , (v 0 − V D ) is integrable for a suitable D ∈ [D 1 , D 0 ]

Theorem

[Blanchet, Bonforte, J.D., Grillo, V´ azquez] Under Assumptions (H1)-(H2), if m < 1 and m 6 = m , the entropy decays according to

F [v (t, · )] ≤ C e 2 (1 m) Λ

α,d

t ∀ t ≥ 0

where Λ α,d > 0 is the best constant in the Hardy–Poincar´e inequality Λ α,d

Z

R

d

| f | 2 dµ α − 1 ≤ Z

R

d

|∇ f | 2 dµ α ∀ f ∈ H 1 (d µ α ) with α := 1/(m − 1) < 0, dµ α := h α dx, h α (x) := (1 + | x | 2 ) α

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Plots ( d = 5)

λ01=−4α−2d

λ10=−2α λ11=−6α−2 (d+ 2) λ02=−8α−4 (d+ 2)

λ20=−4α λ30 λ21λ

12 λ03

λcontα,d:=14(d+ 2α−2)2

α=−d α=−(d+ 2)

α=−d+2 2

α=−d−22 α=−d+62

α 0 Essential spectrum ofLα,d

α=−d−1d2 α=−d−1d+42 α=− d+22

2d (d= 5) Spectrum ofLα,d

mc=d−2d

m1=d−1d m2=d+1d+2

e m1=d+2d

e m2=d+4d+6

m Spectrum of (1−m)L1/(m−1),d

(d= 5)

Essential spectrum of (1

1

m)L1/(m−1),d

2 4 6

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Improved asymptotic rates

[Bonforte, J.D., Grillo, V´ azquez] Assume that m ∈ (m 1 , 1), d ≥ 3.

Under Assumption (H1), if v is a solution of the fast diffusion equation with initial datum v 0 such that R

R

d

x v 0 dx = 0, then the asymptotic convergence holds with an improved rate corresponding to the improved spectral gap.

m1=d+2d

m1=d−1 d

m2=d+4d+6 m2=d+1d+2

4

2

m 1 mc=d−2

d (d= 5)

γ(m)

0

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Higher order matching asymptotics

[J.D., G. Toscani] For some m ∈ (m c , 1) with m c := (d − 2)/d, we consider on R d the fast diffusion equation

∂u

∂τ + ∇ · u ∇ u m 1

= 0

Without choosing R, we may define the function v such that u(τ, y + x 0 ) = R d v (t, x) , R = R(τ) , t = 1 2 log R , x = y

R Then v has to be a solution of

∂v

∂t + ∇ · h v

σ

d2

(m−m

c

) ∇ v m− 1 − 2 x i

= 0 t > 0 , x ∈ R d with (as long as we make no assumption on R)

2 σ

d2

(m−m

c

) = R 1 −d (1 −m) dR dτ

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Refined relative entropy and best matching Barenblatt functions

Consider the family of the Barenblatt profiles B σ (x) := σ

d2

C M + 1 σ | x | 2

m−11

∀ x ∈ R d (1) Note that σ is a function of t : as long as dt 6 = 0, the Barenblatt profile B σ is not a solution (it plays the role of a local Gibbs state) but we may still consider the relative entropy

F σ [v] := 1 m − 1

Z

R

d

v m − B σ m − m B σ m 1 (v − B σ ) dx The time derivative of this relative entropy is

d

dt F σ(t) [v(t , · )] = dσ dt

d dσ F σ [v]

| σ=σ(t)

| {z } choose it = 0

⇐⇒ Minimize F σ [v ] w.r.t. σ ⇐⇒ R

R

d

| x | 2 B σ dx = R

R

d

| x | 2 v dx

+ m

m − 1 Z

R

d

v m− 1 − B σ(t) m 1 ∂v

∂t dx

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Fast diffusion equations:

New points of view (2014-2015)

1

improved inequalities and scalings

2

scalings and a concavity property

3

improved rates and best matching

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Improved inequalities and scalings

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Gagliardo-Nirenberg inequalities and the FDE

k∇ w k ϑ L

2

( R

d

) k w k 1 L

q+1

ϑ ( R

d

) ≥ C GN k w k L

2q

( R

d

)

With the right choice of the constants, the functional J[w ] := 1 4 (q 2 − 1) R

R

d

|∇ w | 2 dx+β R

R

d

| w | q+1 dx −K C α GN R

R

d

| w | 2q dx

2qα

is nonnegative and J[w ] ≥ J[w ] = 0

Theorem

[Dolbeault-Toscani] For some nonnegative, convex, increasing ϕ J[w ] ≥ ϕ

β R

R

d

| w | q+1 dx − R

R

d

| w | q+1 dx for any w ∈ L q+1 ( R d ) such that R

R

d

|∇ w | 2 dx < ∞ and R

R

d

| w | 2q | x | 2 dx = R

R

d

w 2q | x | 2 dx

Consequence for decay rates of relative R´enyi entropies: faster rates of convergence in intermediate asymptotics for ∂u ∂t = ∆u p

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Scalings and a concavity property

⊲ R´enyi entropies, the entropy approach without rescaling: [Savar´e, Toscani]

⊲ faster rates of convergence: [Carrillo, Toscani], [JD, Toscani]

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The fast diffusion equation in original variables

Consider the nonlinear diffusion equation in R d , d ≥ 1

∂u

∂t = ∆u m

with initial datum u(x, t = 0) = u 0 (x) ≥ 0 such that R

R

d

u 0 dx = 1 and R

R

d

| x | 2 u 0 dx < + ∞ . The large time behavior of the solutions is governed by the source-type Barenblatt solutions

U ⋆ (t, x) := 1 κ t 1/µ d B ⋆

x κ t 1/µ

where

µ := 2 + d (m − 1) , κ :=

2 µ m m − 1

1/µ

and B is the Barenblatt profile B (x) :=

C ⋆ − | x | 2 1/(m− 1)

+ if m > 1 C ⋆ + | x | 2 1/(m− 1)

if m < 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The entropy

The entropy is defined by E :=

Z

R

d

u m dx and the Fisher information by

I :=

Z

R

d

u |∇ p | 2 dx with p = m m − 1 u m 1 If u solves the fast diffusion equation, then

E = (1 − m) I To compute I , we will use the fact that

∂p

∂t = (m − 1) p ∆p + |∇ p | 2 F := E σ with σ = µ

d (1 − m) = 1+ 2 1 − m

1

d + m − 1

= 2 d

1 1 − m − 1 has a linear growth asymptotically as t → + ∞

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The concavity property

Theorem

[Toscani-Savar´e] Assume that m ≥ 1 − 1 d if d > 1 and m > 0 if d = 1.

Then F (t) is increasing, (1 − m) F ′′ (t) ≤ 0 and

t→ lim + ∞

1

t F(t ) = (1 − m) σ lim

t→ + ∞ E σ 1 I = (1 − m) σ E σ 1 I ⋆

[Dolbeault-Toscani] The inequality

E σ 1 I ≥ E σ 1 I ⋆

is equivalent to the Gagliardo-Nirenberg inequality k∇ w k θ L

2

( R

d

) k w k 1 L

q+1

θ ( R

d

) ≥ C GN k w k L

2q

( R

d

)

if 1 − 1 d ≤ m < 1. Hint: u m 1/2 = kwk w

L2q(Rd)

, q = 2 m− 1 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The proof

Lemma

If u solves ∂u ∂t = ∆u m with 1 d ≤ m < 1, then I = d

dt Z

R

d

u |∇ p | 2 dx = − 2 Z

R

d

u m

k D 2 p k 2 + (m − 1) (∆p) 2 dx

k D 2 p k 2 = 1

d (∆p) 2 +

D 2 p − 1 d ∆p Id

2

1

σ (1 − m) E 2 σ (E σ ) ′′ = (1 − m) (σ − 1) Z

R

d

u |∇ p | 2 dx 2

− 2 1

d + m − 1 Z

R

d

u m dx Z

R

d

u m (∆p) 2 dx

− 2 Z

R

d

u m dx Z

R

d

u m

D 2 p − 1 d ∆p Id

2

dx

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Best matching

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Relative entropy and best matching

Consider the family of the Barenblatt profiles B σ (x) := σ

d2

C ⋆ + σ 1 | x | 2

m11

∀ x ∈ R d

The Barenblatt profile B σ plays the role of a local Gibbs state if C ⋆ is chosen so that R

R

d

B σ dx = R

R

d

v dx The relative entropy is defined by

F σ [v] := 1 m − 1

Z

R

d

v m − B σ m − m B σ m− 1 (v − B σ ) dx To minimize F σ [v] with respect to σ is equivalent to fix σ such that

σ Z

R

d

| x | 2 B 1 dx = Z

R

d

| x | 2 B σ dx = Z

R

d

| x | 2 v dx

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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A Csisz´ar-Kullback(-Pinsker) inequality

Let m ∈ ( d+2 d , 1) and consider the relative entropy F σ [u] := 1

m − 1 Z

R

d

u m − B σ m − m B σ m− 1 (u − B σ ) dx

Theorem

[J.D., Toscani] Assume that u is a nonnegative function in L 1 ( R d ) such that u m and x 7→ | x | 2 u are both integrable on R d . If k u k L

1

( R

d

) = M and R

R

d

| x | 2 u dx = R

R

d

| x | 2 B σ dx, then F σ [u]

σ

d2

(1 −m) ≥ m 8 R

R

d

B 1 m dx

C ⋆ k u − B σ k L

1

( R

d

) + 1 σ

Z

R

d

| x | 2 | u − B σ | dx 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Temperature (fast diffusion case)

The second moment functional (temperature) is defined by Θ(t ) := 1

d Z

R

d

| x | 2 u(t, x) dx and such that

Θ = 2 E

0 t

τ(0)

τ(t) τ

= lim

s→+∞

τ (s) s Θ

µ/2

(s) s (s τ(0))Θ

s (s

+

τ(t))Θ

µ/2

µ/2

s (s

+

τ

µ/2

s

Fast diffusion case

+

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Temperature (porous medium case) and delay

Let U ⋆ s be the best matching Barenblatt function, in the sense of relative entropy F [u | U ⋆ s ], among all Barenblatt functions ( U ⋆ s ) s>0 . We define s as a function of t and consider the delay given by

τ(t ) :=

Θ(t ) Θ ⋆

µ2

− t

0

s τ(t) τ(0)

τ

= lim

s→+∞

τ(s) t

s (s

+

τ

(0)) Θ

µ/2

s Θ

µ/2

(s)

s (s

+

τ (t))

Θ

µ/2

s (s

+

τ

) Θ

µ/2

Porous medium case

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A result on delays

Theorem

Assume that m ≥ 1 − d 1 and m 6 = 1. The best matching Barenblatt function of a solution u is (t, x) 7→ U (t + τ(t), x) and the function t 7→ τ(t ) is nondecreasing if m > 1 and nonincreasing if 1 − d 1 ≤ m < 1 With G := Θ 1

η2

, η = d (1 − m) = 2 − µ, the R´enyi entropy power functional H := Θ

η2

E is such that

G = µ H with H := Θ

η2

E H

1 − m = Θ 1

η2

Θ I − d E 2

= d E 2

Θ

η2

+1 (q − 1) with q := Θ I d E 2 ≥ 1 d E 2 = 1

d

− Z

R

d

x · ∇ (u m ) dx 2

= 1 d

Z

R

d

x · u ∇ p dx 2

≤ 1 d

Z

R

d

u | x | 2 dx Z

R

d

u |∇ p | 2 dx = Θ I

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Fast diffusion equations on manifolds and sharp functional inequalities

1

The sphere

2

The line

3

Compact Riemannian manifolds

4

The cylinder: Caffarelli-Kohn-Nirenberg inequalities

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Interpolation inequalities on the sphere

Joint work with M.J. Esteban, M. Kowalczyk and M. Loss

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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A family of interpolation inequalities on the sphere

The following interpolation inequality holds on the sphere p − 2

d Z

S

d

|∇ u | 2 d v g + Z

S

d

| u | 2 d v g ≥ Z

S

d

| u | p d v g

2/p

∀ u ∈ H 1 ( S d , dv g ) for any p ∈ (2, 2 ] with 2 = d 2d 2 if d ≥ 3

for any p ∈ (2, ∞ ) if d = 2

Here dv g is the uniform probability measure: v g ( S d ) = 1

1 is the optimal constant, equality achieved by constants p = 2 corresponds to Sobolev’s inequality...

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Stereographic projection

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Sobolev’s inequality

The stereographic projection of S d ⊂ R d × R ∋ (ρ φ, z) onto R d : to ρ 2 + z 2 = 1, z ∈ [ − 1, 1], ρ ≥ 0, φ ∈ S d− 1 we associate x ∈ R d such that r = | x | , φ = | x x |

z = r 2 − 1

r 2 + 1 = 1 − 2

r 2 + 1 , ρ = 2 r r 2 + 1

and transform any function u on S d into a function v on R d using u(y ) = ρ r

d−22

v(x) = r

2

2 +1

d−22

v(x) = (1 − z )

d−22

v(x) p = 2 , S d = 1 4 d (d − 2) | S d | 2/d : Euclidean Sobolev inequality

Z

R

d

|∇ v | 2 dx ≥ S d

Z

R

d

| v |

d2−2d

dx

dd2

∀ v ∈ D 1,2 ( R d )

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Schwarz symmetrization and the ultraspherical setting

(ξ 0 , ξ 1 , . . . ξ d ) ∈ S d , ξ d = z, P d

i=0 | ξ i | 2 = 1 [Smets-Willem]

Lemma

Up to a rotation, any minimizer of Q depends only on ξ d = z

• Let dσ(θ) := (sin Z θ)

dd−1

d θ, Z d := √ π Γ(

d 2 ) Γ( d+1 2 )

: ∀ v ∈ H 1 ([0, π], dσ) p − 2

d Z π

0 | v (θ) | 2 dσ + Z π

0 | v (θ) | 2 d σ ≥ Z π

0 | v (θ) | p

2p

• Change of variables z = cos θ, v(θ) = f (z ) p − 2

d Z 1

− 1 | f | 2 ν dν d + Z 1

− 1 | f | 2 dν d ≥ Z 1

− 1 | f | p dν d

2p

where ν d (z ) dz = dν d (z) := Z d 1 ν

d2

1 dz , ν(z ) := 1 − z 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The ultraspherical operator

With dν d = Z d 1 ν

d2

1 dz, ν(z) := 1 − z 2 , consider the space L 2 (( − 1, 1), dν d ) with scalar product

h f 1 , f 2 i = Z 1

− 1

f 1 f 2 dν d , k f k p = Z 1

− 1

f p dν d

p1

The self-adjoint ultraspherical operator is

L f := (1 − z 2 ) f ′′ − d z f = ν f ′′ + d 2 ν f which satisfies h f 1 , L f 2 i = − R 1

− 1 f 1 f 2 ν dν d

Proposition

Let p ∈ [1, 2) ∪ (2, 2 ], d ≥ 1

−h f , L f i = Z 1

− 1 | f | 2 ν dν d ≥ d k f k 2 p − k f k 2 2

p − 2 ∀ f ∈ H 1 ([ − 1, 1], d ν d )

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Flows on the sphere

Heat flow and the Bakry-Emery method

Fast diffusion (porous media) flow and the choice of the exponents

Joint work with M.J. Esteban, M. Kowalczyk and M. Loss

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Heat flow and the Bakry-Emery method

With g = f p , i.e. f = g α with α = 1/p

(Ineq.) −h f , L f i = −h g α , L g α i =: I [g ] ≥ d k g k 2 1 α − k g 2 α k 1

p − 2 =: F [g ] Heat flow

∂g

∂t = L g d

dt k g k 1 = 0 , d

dt k g 2 α k 1 = − 2 (p − 2) h f , L f i = 2 (p − 2) Z 1

− 1 | f | 2 ν dν d

which finally gives d

dt F [g (t , · )] = − d p − 2

d

dt k g 2 α k 1 = − 2 d I [g (t, · )]

Ineq. ⇐⇒ d

dt F [g (t , · )] ≤ − 2 d F [g (t, · )] ⇐ = d

dt I [g (t, · )] ≤ − 2 d I [g (t , · )]

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The equation for g = f p can be rewritten in terms of f as

∂f

∂t = L f + (p − 1) | f | 2 f ν

− 1 2

d dt

Z 1

− 1 | f | 2 ν dν d = 1 2

d

dt h f , L f i = hL f , L f i + (p − 1) h | f | 2 f ν, L f i d

dt I [g (t, · )] + 2 d I [g (t, · )] = d dt

Z 1

− 1 | f | 2 ν dν d + 2 d Z 1

− 1 | f | 2 ν dν d

= − 2 Z 1

− 1

| f ′′ | 2 + (p − 1) d d + 2

| f | 4

f 2 − 2 (p − 1) d − 1 d + 2

| f | 2 f ′′

f

ν 2 dν d

is nonpositive if

| f ′′ | 2 + (p − 1) d d + 2

| f | 4

f 2 − 2 (p − 1) d − 1 d + 2

| f | 2 f ′′

f is pointwise nonnegative, which is granted if

(p − 1) d − 1 d + 2

2

≤ (p − 1) d

d + 2 ⇐⇒ p ≤ 2 d 2 + 1

(d − 1) 2 = 2 # < 2 d d − 2 = 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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... up to the critical exponent: a proof in two slides

d dz , L

u = ( L u) − L u = − 2 z u ′′ − d u Z 1

− 1

( L u) 2 dν d = Z 1

− 1 | u ′′ | 2 ν 2 d ν d + d Z 1

− 1 | u | 2 ν dν d

Z 1

− 1

( L u) | u | 2

u ν dν d = d d + 2

Z 1

− 1

| u | 4

u 2 ν 2 dν d − 2 d − 1 d + 2

Z 1

− 1

| u | 2 u ′′

u ν 2 dν d

On ( − 1, 1), let us consider the porous medium (fast diffusion) flow u t = u 2

L u + κ | u | 2 u ν

If κ = β (p − 2) + 1, the L p norm is conserved d

dt Z 1

− 1

u βp dν d = β p (κ − β (p − 2) − 1) Z 1

− 1

u β(p 2) | u | 2 ν dν d = 0

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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f = u β , k f k 2 L

2

( S

d

) + p d 2

k f k 2 L

2

( S

d

) − k f k 2 L

p

( S

d

)

≥ 0 ?

A :=

Z 1

− 1 | u ′′ | 2 ν 2 dν d − 2 d − 1

d + 2 (κ + β − 1) Z 1

− 1

u ′′ | u | 2 u ν 2 dν d

+

κ (β − 1) + d

d + 2 (κ + β − 1) Z 1

− 1

| u | 4 u 2 ν 2 dν d

A is nonnegative for some β if 8 d 2

(d + 2) 2 (p − 1) (2 − p) ≥ 0

A is a sum of squares if p ∈ (2, 2 ) for an arbitrary choice of β in a certain interval (depending on p and d)

A = Z 1

− 1

u ′′ − p + 2 6 − p

| u | 2 u

2

ν 2 dν d ≥ 0 if p = 2 and β = 4 6 − p

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(51)

The rigidity point of view

Which computation have we done ? u t = u 2

L u + κ |u

|

2

u ν

− L u − (β − 1) | u | 2

u ν + λ

p − 2 u = λ p − 2 u κ Multiply by L u and integrate

...

Z 1

− 1 L u u κ dν d = − κ Z 1

− 1

u κ | u | 2 u dν d

Multiply by κ | u

|

2

u and integrate ... = + κ

Z 1

− 1

u κ | u | 2 u dν d

The two terms cancel and we are left only with the two-homogenous terms

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(52)

Improvements of the inequalities (subcritical range)

as long as the exponent is either in the range (1, 2) or in the range (2, 2 ), on can establish improved inequalities

An improvement automatically gives an explicit stability result of the optimal functions in the (non-improved) inequality

By duality, this provides a stability result for Keller-Lieb-Tirring inequalities

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(53)

What does “improvement” mean ?

An improved inequality is

d Φ (e) ≤ i ∀ u ∈ H 1 ( S d ) s.t. k u k 2 L

2

( S

d

) = 1 for some function Φ such that Φ(0) = 0, Φ (0) = 1, Φ > 0 and Φ(s) > s for any s. With Ψ(s) := s − Φ 1 (s)

i − d e ≥ d (Ψ ◦ Φ)(e) ∀ u ∈ H 1 ( S d ) s.t. k u k 2 L

2

( S

d

) = 1 Lemma (Generalized Csisz´ar-Kullback inequalities)

k∇ u k 2 L

2

( S

d

) − d p − 2

h k u k 2 L

p

( S

d

) − k u k 2 L

2

( S

d

)

i

≥ d k u k 2 L

2

( S

d

) (Ψ ◦ Φ)

C k u k

2 (1−r) Ls(Sd)

k u k

2L2 (Sd)

k u r − u ¯ r k 2 L

q

( S

d

)

∀ u ∈ H 1 ( S d ) s(p) := max { 2, p } and p ∈ (1, 2): q(p) := 2/p, r (p) := p; p ∈ (2, 4):

q = p/2, r = 2; p ≥ 4: q = p/(p − 2), r = p − 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(54)

Linear flow: improved Bakry-Emery method

Cf. [Arnold, JD]

w t = L w + κ | w | 2 w ν With 2 := (d− 2 d

2

+1 1)

2

γ 1 :=

d − 1 d + 2

2

(p − 1) (2 # − p) if d > 1 , γ 1 := p − 1

3 if d = 1 If p ∈ [1, 2) ∪ (2, 2 ] and w is a solution, then

d

dt (i − d e) ≤ − γ 1

Z 1

− 1

| w | 4

w 2 dν d ≤ − γ 1 | e | 2 1 − (p − 2) e Recalling that e = − i, we get a differential inequality

e ′′ + d e ≥ γ 1 | e | 2 1 − (p − 2) e After integration: d Φ(e(0)) ≤ i(0)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Nonlinear flow: the H¨older estimate of J. Demange

w t = w 2

L w + κ | w | 2 w

For all p ∈ [1, 2 ], κ = β (p − 2) + 1, dt d R 1

− 1 w βp dν d = 0

1

2

dt d R 1

− 1

| (w β ) | 2 ν + p d 2 w − w

dν d ≥ γ R 1

− 1

|w

|

4

w

2

ν 2 dν d

Lemma

For all w ∈ H 1 ( − 1, 1), dν d

, such that R 1

− 1 w βp dν d = 1 Z 1

− 1

| w | 4

w 2 ν 2 dν d ≥ 1 β 2

R 1

− 1 | (w β ) | 2 ν d ν d

R 1

− 1 | w | 2 ν dν d

R 1

− 1 w dν d

δ

.... but there are conditions on β

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(56)

Admissible ( p, β ) for d = 5

0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0

1 2 3 4 5 6

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(57)

The line

A first example of a non-compact manifold

Joint work with M.J. Esteban, A. Laptev and M. Loss

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(58)

One-dimensional Gagliardo-Nirenberg-Sobolev inequalities

k f k L

p

( R ) ≤ C GN (p) k f k θ L

2

( R ) k f k 1 L

2

( θ R ) if p ∈ (2, ∞ ) k f k L

2

( R ) ≤ C GN (p) k f k η L

2

( R ) k f k 1 L

p

( η R ) if p ∈ (1, 2) with θ = p 2 p 2 and η = 2 2+p p

The threshold case corresponding to the limit as p → 2 is the logarithmic Sobolev inequality

R

R u 2 log

u

2

k u k

2L2 (R)

dx ≤ 1 2 k u k 2 L

2

( R ) log

2 π e

ku

k

2L2 (R)

k u k

2L2 (R)

If p > 2, u ⋆ (x) = (cosh x)

p22

solves

− (p − 2) 2 u ′′ + 4 u − 2 p | u | p− 2 u = 0 If p ∈ (1, 2) consider u (x) = (cos x)

22p

, x ∈ ( − π/2, π/2)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Flow

Let us define on H 1 ( R ) the functional F [v] := k v k 2 L

2

( R ) + 4

(p − 2) 2 k v k 2 L

2

( R ) − C k v k 2 L

p

( R ) s.t. F [u ⋆ ] = 0 With z (x) := tanh x , consider the flow

v t = v 1

p2

√ 1 − z 2

v ′′ + 2 p

p − 2 z v + p 2

| v | 2

v + 2

p − 2 v

Theorem (Dolbeault-Esteban-Laptev-Loss) Let p ∈ (2, ∞ ). Then

d

dt F [v(t)] ≤ 0 and lim

t →∞ F [v(t)] = 0

d

dt F [v (t )] = 0 ⇐⇒ v 0 (x) = u ⋆ (x − x 0 ) Similar results for p ∈ (1, 2)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(60)

The inequality ( p > 2) and the ultraspherical operator

The problem on the line is equivalent to the critical problem for the ultraspherical operator

Z

R

| v | 2 dx + 4 (p − 2) 2

Z

R

| v | 2 dx ≥ C Z

R

| v | p dx

2p

With

z (x) = tanh x , v ⋆ = (1 − z 2 )

p12

and v (x) = v ⋆ (x ) f (z(x)) equality is achieved for f = 1 and, if we let ν(z ) := 1 − z 2 , then

Z 1

− 1 | f | 2 ν d ν d + 2 p (p − 2) 2

Z 1

− 1 | f | 2 dν d ≥ 2 p (p − 2) 2

Z 1

− 1 | f | p dν d

2p

where dν p denotes the probability measure dν p (z ) := ζ 1

p

ν

p22

dz d = p− 2 p 2 ⇐⇒ p = d− 2d 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(61)

Change of variables = stereographic projection + Emden-Fowler

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(62)

Compact Riemannian manifolds

no sign is required on the Ricci tensor and an improved integral criterion is established

the flow explores the energy landscape... and shows the non-optimality of the improved criterion

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(63)

Riemannian manifolds with positive curvature

( M , g ) is a smooth closed compact connected Riemannian manifold dimension d, no boundary, ∆ g is the Laplace-Beltrami operator vol( M ) = 1, R is the Ricci tensor, λ 1 = λ 1 ( − ∆ g )

ρ := inf

M inf

ξ ∈ S

d−1

R (ξ , ξ) Theorem (Licois-V´eron, Bakry-Ledoux)

Assume d ≥ 2 and ρ > 0. If λ ≤ (1 − θ) λ 1 + θ d ρ

d − 1 where θ = (d − 1) 2 (p − 1) d (d + 2) + p − 1 > 0 then for any p ∈ (2, 2 ), the equation

− ∆ g v + λ

p − 2 v − v p− 1

= 0 has a unique positive solution v ∈ C 2 ( M ): v ≡ 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Riemannian manifolds: first improvement

Theorem (Dolbeault-Esteban-Loss) For any p ∈ (1, 2) ∪ (2, 2 )

0 < λ < λ ⋆ = inf

u∈ H

2

(M)

Z

M

h (1 − θ) (∆ g u) 2 + θ d

d − 1 R ( ∇ u, ∇ u) i d v g

R

M |∇ u | 2 d v g

there is a unique positive solution in C 2 ( M ): u ≡ 1 lim p → 1

+

θ(p) = 0 = ⇒ lim p → 1

+

λ ⋆ (p) = λ 1 if ρ is bounded λ ⋆ = λ 1 = d ρ/(d − 1) = d if M = S d since ρ = d − 1

(1 − θ) λ 1 + θ d ρ

d − 1 ≤ λ ⋆ ≤ λ 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(65)

Riemannian manifolds: second improvement

H g u denotes Hessian of u and θ = (d − 1) 2 (p − 1) d (d + 2) + p − 1 Q g u := H g u − g

d ∆ g u − (d − 1) (p − 1) θ (d + 3 − p)

∇ u ⊗ ∇ u

u − g

d

|∇ u | 2 u

Λ ⋆ := inf

u ∈ H

2

( M ) \{ 0 }

(1 − θ) Z

M

(∆ g u) 2 d v g + θ d d − 1

Z

M

h k Q g u k 2 + R ( ∇ u, ∇ u) i Z

M |∇ u | 2 d v g

Theorem (Dolbeault-Esteban-Loss)

Assume that Λ ⋆ > 0. For any p ∈ (1, 2) ∪ (2, 2 ), the equation has a unique positive solution in C 2 ( M ) if λ ∈ (0, Λ ⋆ ): u ≡ 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Optimal interpolation inequality

For any p ∈ (1, 2) ∪ (2, 2 ) or p = 2 if d ≥ 3 k∇ v k 2 L

2

(M) ≥ λ

p − 2 h

k v k 2 L

p

(M) − k v k 2 L

2

(M)

i

∀ v ∈ H 1 ( M ) Theorem (Dolbeault-Esteban-Loss)

Assume Λ ⋆ > 0. The above inequality holds for some λ = Λ ∈ [Λ ⋆ , λ 1 ] If Λ ⋆ < λ 1 , then the optimal constant Λ is such that

Λ ⋆ < Λ ≤ λ 1

If p = 1, then Λ = λ 1

Using u = 1 + ε ϕ as a test function where ϕ we get λ ≤ λ 1

A minimum of

v 7→ k∇ v k 2 L

2

(M) − p λ 2 h

k v k 2 L

p

(M) − k v k 2 L

2

(M)

i

under the constraint k v k L

p

( M ) = 1 is negative if λ > λ 1

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(67)

The flow

The key tools the flow u t = u 2

∆ g u + κ |∇ u | 2 u

, κ = 1 + β (p − 2) If v = u β , then dt d k v k L

p

(M) = 0 and the functional

F [u] :=

Z

M |∇ (u β ) | 2 d v g + λ p − 2

"Z

M

u 2 β d v g − Z

M

u β p d v g

2/p #

is monotone decaying

J. Demange, Improved Gagliardo-Nirenberg-Sobolev inequalities on manifolds with positive curvature, J. Funct. Anal., 254 (2008), pp. 593–611. Also see C. Villani, Optimal Transport, Old and New

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Elementary observations (1/2)

Let d ≥ 2, u ∈ C 2 ( M ), and consider the trace free Hessian L g u := H g u − g

d ∆ g u Lemma

Z

M

(∆ g u) 2 d v g = d d − 1

Z

M

k L g u k 2 d v g + d d − 1

Z

M

R ( ∇ u, ∇ u) d v g

Based on the Bochner-Lichnerovicz-Weitzenb¨ ock formula 1

2 ∆ |∇ u | 2 = k H g u k 2 + ∇ (∆ g u) · ∇ u + R ( ∇ u, ∇ u)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Elementary observations (2/2)

Lemma

Z

M

∆ g u |∇ u | 2 u d v g

= d

d + 2 Z

M

|∇ u | 4

u 2 d v g − 2 d d + 2

Z

M

[L g u] :

∇ u ⊗ ∇ u u

d v g

Lemma

Z

M

(∆ g u) 2 d v g ≥ λ 1

Z

M

|∇ u | 2 d v g ∀ u ∈ H 2 ( M ) and λ 1 is the optimal constant in the above inequality

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The key estimates

G [u] := R

M

h θ (∆ g u) 2 + (κ + β − 1) ∆ g u |∇u| u

2

+ κ (β − 1) |∇u| u

24

i d v g

Lemma 1 2 β 2

d

dt F [u] = − (1 − θ) Z

M

(∆ g u) 2 d v g − G [u] + λ Z

M

|∇ u | 2 d v g

Q θ g u := L g u − 1 θ d d+2 1 (κ + β − 1) h

∇ u ⊗∇ u

u − g d |∇u| u

2

i Lemma

G [u] = θ d d − 1

Z

M k Q θ g u k 2 d v g + Z

M

R ( ∇ u, ∇ u) d v g

− µ Z

M

|∇ u | 4 u 2 d v g

with µ := 1 θ

d − 1 d + 2

2

(κ + β − 1) 2 − κ (β − 1) − (κ + β − 1) d d + 2

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The end of the proof

Assume that d ≥ 2. If θ = 1, then µ is nonpositive if β (p) ≤ β ≤ β + (p) ∀ p ∈ (1, 2 ) where β ± := b ± 2 a b

2

a with a = 2 − p + h

(d− 1) (p− 1) d+2

i 2

and b = d+3 d+2 p Notice that β (p) < β + (p) if p ∈ (1, 2 ) and β (2 ) = β + (2 )

θ = (d − 1) 2 (p − 1)

d (d + 2) + p − 1 and β = d + 2 d + 3 − p Proposition

Let d ≥ 2, p ∈ (1, 2) ∪ (2, 2 ) (p 6 = 5 or d 6 = 2) 1

2 β 2 d

dt F [u] ≤ (λ − Λ ⋆ ) Z

M

|∇ u | 2 d v g

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(72)

The Moser-Trudinger-Onofri inequality on Riemannian manifolds

Joint work with G. Jankowiak and M.J. Esteban

Extension to compact Riemannian manifolds of dimension 2...

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(73)

We shall also denote by R the Ricci tensor, by H g u the Hessian of u and by

L g u := H g u − g d ∆ g u

the trace free Hessian. Let us denote by M g u the trace free tensor M g u := ∇ u ⊗ ∇ u − g

d |∇ u | 2 We define

λ ⋆ := inf

u ∈ H

2

( M ) \{ 0 }

Z

M

h

k L g u − 1 2 M g u k 2 + R ( ∇ u, ∇ u) i

e u/2 d v g

Z

M |∇ u | 2 e u/2 d v g

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(74)

Theorem

Assume that d = 2 and λ ⋆ > 0. If u is a smooth solution to

− 1

2 ∆ g u + λ = e u then u is a constant function if λ ∈ (0, λ ⋆ ) The Moser-Trudinger-Onofri inequality on M

1

4 k∇ u k 2 L

2

( M ) + λ Z

M

u d v g ≥ λ log Z

M

e u d v g

∀ u ∈ H 1 ( M ) for some constant λ > 0. Let us denote by λ 1 the first positive eigenvalue of − ∆ g

Corollary

If d = 2, then the MTO inequality holds with λ = Λ := min { 4 π, λ ⋆ } . Moreover, if Λ is strictly smaller than λ 1 /2, then the optimal constant in the MTO inequality is strictly larger than Λ

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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The flow

∂f

∂t = ∆ g (e −f /2 ) − 1 2 |∇ f | 2 e −f /2 G λ [f ] :=

Z

M k L g f − 1 2 M g f k 2 e f /2 d v g + Z

M

R ( ∇ f , ∇ f ) e f /2 d v g

− λ Z

M

|∇ f | 2 e f /2 d v g Then for any λ ≤ λ ⋆ we have

d

dt F λ [f (t, · )] = Z

M − 1 2 ∆ g f + λ ∆ g (e f /2 ) − 1 2 |∇ f | 2 e f /2 d v g

= − G λ [f (t , · )]

Since F λ is nonnegative and lim t→∞ F λ [f (t, · )] = 0, we obtain that F λ [u] ≥

Z

0 G λ [f (t , · )] dt

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(76)

Weighted Moser-Trudinger-Onofri inequalities on the two-dimensional Euclidean space

On the Euclidean space R 2 , given a general probability measure µ does the inequality

1 16 π

Z

R

2

|∇ u | 2 dx ≥ λ

log Z

R

d

e u

− Z

R

d

u dµ

hold for some λ > 0 ? Let

Λ ⋆ := inf

x ∈ R

2

− ∆ log µ 8 π µ Theorem

Assume that µ is a radially symmetric function. Then any radially symmetric solution to the EL equation is a constant if λ < Λ ⋆ and the inequality holds with λ = Λ ⋆ if equality is achieved among radial functions

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(77)

Caffarelli-Kohn-Nirenberg inequalities

A sketch of the proof —

In collaboration with M.J. Esteban and M. Loss

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

(78)

a b

0

− 1

1

b = a + 1

b = a b = b

FS

(a)

b = b

direct

(a) Symmetry region

Symmetry breaking region

a

c

=

d−22

The Felli-Schneider region, or symmetry breaking region, appears in dark grey and is defined by a < 0, a ≤ b < b

FS

(a). We prove that symmetry holds in the light grey region defined by b ≥ b

FS

(a) when a < 0 and for any b ∈ [a, a + 1] if a ∈ [0, a

c

)

J. Dolbeault Sharp functional inequalities and nonlinear diffusions

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Although this approach is restricted to radially symmetric functions, one of the most striking way to justify the fact that the Onofri inequality plays in dimension two a role

⊲ Stability of entropy – entropy production inequalities (scaling methods), and improved rates of convergence [Carrillo, Toscani], [J.D., Toscani]... Range of

Fast diffusion equations: new points of view Fast diffusion equations on manifolds and sharp functional inequalities Introduction to symmetry breaking in