Curvature and Diffusion in the Heisenberg group Nicolas JUILLET - - PowerPoint PPT Presentation

curvature and diffusion in the heisenberg group
SMART_READER_LITE
LIVE PREVIEW

Curvature and Diffusion in the Heisenberg group Nicolas JUILLET - - PowerPoint PPT Presentation

Curvature and Diffusion in the Heisenberg group Curvature and Diffusion in the Heisenberg group Nicolas JUILLET IRMA, Strasbourg Paris, IHP , October 2014 Nicolas JUILLET Curvature and Diffusion in the Heisenberg group Curvature and


slide-1
SLIDE 1

Curvature and Diffusion in the Heisenberg group

Curvature and Diffusion in the Heisenberg group

Nicolas JUILLET

IRMA, Strasbourg

Paris, IHP , October 2014

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-2
SLIDE 2

Curvature and Diffusion in the Heisenberg group

Outline

1

Notations and definitions

2

Curvature

3

Diffusion

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-3
SLIDE 3

Curvature and Diffusion in the Heisenberg group Notations and definitions

The subRiemannian H.

A basis for left-invariant vector fields is X = E1 − y 2 E3 , Y = E2 + x 2 E3 and Z = [X,Y] = E3. A curve is horizontal if ˙

γ ∈ Vect(X,Y) for any t. Actually ˙ γ(t) = a(t)X(γ(t))+ b(t)Y(γ(t)).

It has norm |˙

γ| =

  • a2(t)+ b2(t) and the length of γ is

γ|.

The diffusion operator is ∆ = X2 + Y2. The horizontal gradient is

∇f = XfX+ YfY.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-4
SLIDE 4

Curvature and Diffusion in the Heisenberg group Notations and definitions

The Riemannian Hε for ε > 0

Let ε > 0 and Hε := (R3,dε,L3). An orthonormal basis at point (x,y,u) is X = E1 − y 2 E3 , Y = E2 + x 2 E3 and

εZ = ε[X,Y] = εE3.

If

˙ γ(t) = (a(t)X+ b(t)Y+ c(t)Z)(γ(t))

then |˙

γ(t)|ε =

  • a2 + b2 + c2

ε2 and lengthε(γ) =

a2 + b2 + c2

ε2 (t)dt.

The gradient is ∇εf = ∇f +(ε2Zf)Z.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-5
SLIDE 5

Curvature and Diffusion in the Heisenberg group Notations and definitions

Curves in P2(X).

For a metric measure space (X,d,ν), two theories make use of curves in the space

  • f probability measures P2(X) endowed with the transport distance W.

Ricci bounds: geodesic curves. (Lott-Villani and Sturm) Heat diffusion: curves with maximal slope. (Ambrosio-Gigli-Savaré)

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-6
SLIDE 6

Curvature and Diffusion in the Heisenberg group Notations and definitions

Comparaison of the Wasserstein distances

Let W be the L2-minimal metric with respect to the Carnot-Carathéodory metric dCC and Wε with respect to dε. Wε ≤ W,

P2(H) = P2(Hε) as topological spaces.

Lipschitz curves (resp. absolutely continuous) of P2(H) are Lipschitz (resp. absolutely continuous) in P2(Hε).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-7
SLIDE 7

Curvature and Diffusion in the Heisenberg group Notations and definitions

Geodesic curves

Theorem (Ambrosio-Rigot, 2004) Let µ0,µ1 ∈ P2(H) such that µ0 is absolutely continuous. Then there is a unique

  • ptimal coupling π. It is π = (Id⊗T)#µ0 for some map T. Moreover there is a unique

geodesic between p and T(p) (µ0-almost surely). In fact T(p) = p.expH(∇ψ(p),Zψ(p)). Here ψ : H → R depends on µ0,µ1. The unique geodesic (µs)s∈[0,1] between µ0 and µ1 is defined by µs = (Ts)#µ0 where Ts(p) = p.expH(s∇ψ(p),sZψ(p)).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-8
SLIDE 8

Curvature and Diffusion in the Heisenberg group Notations and definitions

Absolutely continuous curves

Theorem Let (µt)t∈[0,T] be an absolutely continuous curve of P2(H). Then for almost every t > 0 there exists a field of horizontal vectors vt ∈ TanµtP2(H) such that the continuity equation is satisfied dµt/dt + div(vtµt) = 0. Moreover

|vt|2dµt = limh→0+ h−1W(µt,µt+h) =: Speed(µt).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-9
SLIDE 9

Curvature and Diffusion in the Heisenberg group Notations and definitions

The relative entropy

The relative entropy of µ = ρL is given by H(µ) = H(µ | L) =

  • ρln(ρ)(x)dL(x).

Big entropy: µ concentrated on a few space. Small entropy: µ take a lot of space.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-10
SLIDE 10

Curvature and Diffusion in the Heisenberg group Curvature

Ricci curvature bounds on a Riemannian manifolds

Theorem Let (M,g) be a Riemannian manifold of dimension N and K ∈ R. Then the following properties are equivalent.

1

∀(x,v) ∈ TM, Ricci(v,v) ≥ Kg(v,v)

2

∀f ∈ C∞(M),∀x ∈ M, Γ2(f)(x) ≥ KΓ(f)(x)+(∆f(x))2/N

3

(M,dg,volg) satisfies the Curvature Dimension Condition CD(K,N),

4

(M,dg,volg) satisfies the Measure Contraction Property MCP(K,N)

Under this condition, one can deduce a lot of analytico-geometric results.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-11
SLIDE 11

Curvature and Diffusion in the Heisenberg group Curvature

MCP is satisfied

Jacobian estimate For any e ∈ H. The contraction map M s

e : f → M s(e,f) is differentiable with

Jac(M s

e )(f) ≥ s5.

Equality case : e and f are on a horizontal line. As a consequence (H,dc,L3) satisfies MCP(0,5): Measure Contraction Property MCP(0,N) for (X,d,ν): for every point e ∈ X and for all s ∈ [0,1],

M s

e #ν ≤ sNν.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-12
SLIDE 12

Curvature and Diffusion in the Heisenberg group Curvature

K-convexity and Ricci curvature

Theorem (Cordero–McCann–Schmuckenschläger and Sturm–von Renesse) Let M be a Riemannian manifold. It has Ricci curvature bounded from below by K ∈ R if and only if for every geodesic

(µt)t∈[0,T] in P2(M) of speed 1 the function

t ∈ [0,T] → H(µt | VolM)− K.t2 2 ∈ R is convex. This theorem has been turned into the definition of CD(K,+∞) for metric measure spaces: A space satisfies CD(K,+∞) if H(.|ν) is K-convex along every geodesic curve of (P2(X),Wd).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-13
SLIDE 13

Curvature and Diffusion in the Heisenberg group Curvature

The curvature dimension condition is not satisfied.

Theorem (J.) In P2(H) the entropy H with respect to L is not K-convex along geodesics (for any K ∈ R). The curvature-dimension conditions introduced by Lott–Villani and Sturm are not satisfied

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-14
SLIDE 14

Curvature and Diffusion in the Heisenberg group Curvature

The general theorem is Theorem (J. 2009) In (Hn,L2n+1,dc), the Heisenberg group with the Lebesgue measure and the Carnot-Carathéodory distance, MCP(K,N) is true if and only if N ≥ 2n + 3 and K ≤ 0, CD(K,N) is false for every (K,N).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-15
SLIDE 15

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′

E F Let F be a small ball such that 0H and the center of the ball are on a “bad" geodesic. For E we take the “geodesic inverse" of F.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-16
SLIDE 16

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′

E F Let F be a small ball such that 0H and the center of the ball are on a “bad" geodesic. For E we take the “geodesic inverse" of F. It turns out that L(E) = L(F). We want to prove L

  • M 1/2(E,F)
  • < L(F) because it is a contradiction to the

Brunn-Minkowski inequality.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-17
SLIDE 17

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′ For each e ∈ E, the contracted set M 1/2(e,F) is a sort of ellipsoid that contains 0H. The volume of such an ellipsoid is 2−5L(F).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-18
SLIDE 18

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′ For each e ∈ E, the contracted set M 1/2(e,F) is a sort of ellipsoid that contains 0H. The volume of such an ellipsoid is 2−5L(F).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-19
SLIDE 19

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′ For each e ∈ E, the contracted set M 1/2(e,F) is a sort of ellipsoid that contains 0H. The volume of such an ellipsoid is 2−5L(F).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-20
SLIDE 20

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′ The midset M 1/2(E,F) is made of the reunion of these ellipsoids.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-21
SLIDE 21

Curvature and Diffusion in the Heisenberg group Curvature

Sketch of proof

p p′ 0H a b b′ a′ All of them contains 0H. Then M 1/2(E,F) is an ellipsoid of size 2. Its volume is 23

·2−5L(F)

  • = L(F)

4

.

Then L(M 1/2) < L(F) = L(E).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-22
SLIDE 22

Curvature and Diffusion in the Heisenberg group Diffusion

After Jordan-Kinderlehrer-Otto (2000) “The heat flow is the gradient flow of H in P2(X)" Gradient flow means ˙

γt = −∇F(γt). We need a metric definition of this equation.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-23
SLIDE 23

Curvature and Diffusion in the Heisenberg group Diffusion

Gradient flow of the relative entropy.

An absolutely continuous curve (µt)t≥0 is a gradient flow of H if t → H(µt) is decreasing. for almost every t > 0,

   ∂tH(µt) = −Speed(µt)· Slope(H)(µt)

Speed(µt) = Slope(H)(µt). Theorem (J. 2014) If the curve (µt)t>0 is a gradient flow of H then µt = ρtL3 and

∂ ∂t ρt = ∆ρt.

The converse is true.

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-24
SLIDE 24

Curvature and Diffusion in the Heisenberg group Diffusion

Is Slope(µ) the same as

  • I(µ) =

|∇ρ|2/ρdL ?

In the Riemannian setting we have Slopeε(µ) =

I +ε2J where J(µ) = (Zρ)2/ρdL

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-25
SLIDE 25

Curvature and Diffusion in the Heisenberg group Diffusion

HWI inequalities in measures with finite Riemannian slope

We can go from the HWI inequality H(ν) ≥ H(µ)−

  • Iε(µ)Wε(µ,ν)+ 1

2 ·

−1

2ε2

  • Wε(µ,ν)2

that is available in Hε for every ε > 0 to H(ν) ≥ H(µ)−

  • I(µ)W(µ,ν)− C(µ)W(µ,ν)3/2,

but only if Iε(µ) = I(µ)+ε2J(µ) is finite (and C = (J/2I)+ 1/4).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-26
SLIDE 26

Curvature and Diffusion in the Heisenberg group Diffusion

Slopeε =

I +ε2J is an upper gradient of H on P2(Hε)

With the following Riemannian result Upper gradient on the Riemannian Hε Let (µt)t≥0 be an absolutely continuous curve of P2(Hε). If t1

t0

Slopeε(H)(µt)Speedε(µt) < +∞ then t → H(µt) is absolutely continuous. Moreover

|H(µt0)− H(µt1)| ≤

t1

t0

  • Iε(µt)Speedε(µt)dt.

We can prove that

I (≤ Slope(H)) is an upper gradient of H in P2(H).

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group

slide-27
SLIDE 27

Curvature and Diffusion in the Heisenberg group Diffusion

Theorem (Ambrosio-Gigli-Savaré 2014)

µt = ρtν is a gradient flow of H(.|ν) in P2(X) if and only if ft is a gradient flow of the

Dirichlet-Cheeger energy in L2(X,ν). It holds without any assumption on (X,d,ν) but the heat flow can be degenerate, non-unique, non-linear. A good additional assumption is that the space satisfies RCD∗(K,N). A large part of the theory holds for Carnot groups

Nicolas JUILLET Curvature and Diffusion in the Heisenberg group