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Lipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin Prairie Analysis Seminar Kansas State University September 25, 2015 Joint work with Maria Colombo and Alessio Figalli. Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 1 / 16

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Page 1: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Lipschitz Changes of Variables between Perturbations ofLog-concave Measures

Yash Jhaveri

University of Texas at Austin

Prairie Analysis SeminarKansas State University

September 25, 2015

Joint work with Maria Colombo and Alessio Figalli.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 1 / 16

Page 2: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

An Old Result

Theorem (Caffarelli)

Let Q be a quadratic polynomial with D2Q > 0 and V be a convexfunction such that e−Q , e−Q−V ∈ P(Rn). Then, there exists a1-Lipschitz change of variables T taking e−Q to e−Q−V .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 2 / 16

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A New Result

Theorem (Colombo, Figalli, -)

Let V be a convex function with V (0) = inf V , R > 0, q ∈ Cc(BR), and cq ∈ Rbe such that e−V , e−V+cq−q ∈ P(Rn). Assume that λ Id ≤ D2V ≤ Λ Id andD2q ≥ −λq Id for 0 < λ,Λ, λq <∞ in the sense of distributions. Then, thereexists a change of variables T taking e−V to e−V+cq−q that satisfies

‖∇T‖L∞(Rn) ≤ C with C = C (R, λ,Λ, λq) > 0

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 3 / 16

Page 4: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Existence: The Optimal Transport Problem

- The map T is the unique solution of the Monge problem forquadratic cost:

min

{∫Rn

|x − T (x)|2 dµ(x) : T#µ = ν

},

where µ = e−V (x) dx , ν = e−V (y)+cq−q(y) dy ∈ P(Rn).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 4 / 16

Page 5: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Brenier’s Theorem

Theorem (Brenier)

Let µ, ν ∈ P(Rn) such that µ = f (x) dx and∫Rn

|x |2 dµ(x) +

∫Rn

|y |2 dν(y) <∞.

Then, there exists a unique, optimal transport T taking µ to ν.Moreover, there is a convex function φ : Rn → R such that

T = ∇φ.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 5 / 16

Page 6: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Regularity: OT and the Monge-Ampere Equation

- Let µ = f (x) dx , ν = g(y) dy ∈ P(Rn), ϕ ∈ C∞c (Rn), andassume that the OT map T taking f to g is a smoothdiffeomorphism.

Then,∫ϕ(T (x))f (x) dx

T#µ=ν=

∫ϕ(y)g(y) dy

y=T (x)=

∫ϕ(T (x))g(T (x))| det∇T (x)| dx .

- Since ϕ ∈ C∞c (Rn) was arbitrary,

f (x) = g(T (x))| det∇T (x)|.

- Recalling Brenier, if g > 0,

detD2φ =f

g(∇φ).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 6 / 16

Page 7: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Regularity: OT and the Monge-Ampere Equation

- Let µ = f (x) dx , ν = g(y) dy ∈ P(Rn), ϕ ∈ C∞c (Rn), andassume that the OT map T taking f to g is a smoothdiffeomorphism. Then,∫

ϕ(T (x))f (x) dxT#µ=ν

=

∫ϕ(y)g(y) dy

y=T (x)=

∫ϕ(T (x))g(T (x))| det∇T (x)| dx .

- Since ϕ ∈ C∞c (Rn) was arbitrary,

f (x) = g(T (x))| det∇T (x)|.

- Recalling Brenier, if g > 0,

detD2φ =f

g(∇φ).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 6 / 16

Page 8: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Regularity: OT and the Monge-Ampere Equation

- Let µ = f (x) dx , ν = g(y) dy ∈ P(Rn), ϕ ∈ C∞c (Rn), andassume that the OT map T taking f to g is a smoothdiffeomorphism. Then,∫

ϕ(T (x))f (x) dxT#µ=ν

=

∫ϕ(y)g(y) dy

y=T (x)=

∫ϕ(T (x))g(T (x))| det∇T (x)| dx .

- Since ϕ ∈ C∞c (Rn) was arbitrary,

f (x) = g(T (x))| det∇T (x)|.

- Recalling Brenier, if g > 0,

detD2φ =f

g(∇φ).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 6 / 16

Page 9: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Regularity: OT and the Monge-Ampere Equation

- Let µ = f (x) dx , ν = g(y) dy ∈ P(Rn), ϕ ∈ C∞c (Rn), andassume that the OT map T taking f to g is a smoothdiffeomorphism. Then,∫

ϕ(T (x))f (x) dxT#µ=ν

=

∫ϕ(y)g(y) dy

y=T (x)=

∫ϕ(T (x))g(T (x))| det∇T (x)| dx .

- Since ϕ ∈ C∞c (Rn) was arbitrary,

f (x) = g(T (x))| det∇T (x)|.

- Recalling Brenier, if g > 0,

detD2φ =f

g(∇φ).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 6 / 16

Page 10: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since T = ∇φ and φ is convex, we know that φαα ≥ 0 for everydirection α.

- So, we just need to find an upper bound on φαα.

- Let’s assume that φαα attains a global maximum at some pointx0 ∈ Rn, and without loss of generality, assume that this happensin the e1-direction.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 7 / 16

Page 11: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since T = ∇φ and φ is convex, we know that φαα ≥ 0 for everydirection α.

- So, we just need to find an upper bound on φαα.

- Let’s assume that φαα attains a global maximum at some pointx0 ∈ Rn, and without loss of generality, assume that this happensin the e1-direction.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 7 / 16

Page 12: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since T = ∇φ and φ is convex, we know that φαα ≥ 0 for everydirection α.

- So, we just need to find an upper bound on φαα.

- Let’s assume that φαα attains a global maximum at some pointx0 ∈ Rn, and without loss of generality, assume that this happensin the e1-direction.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 7 / 16

Page 13: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since our potential φ solves a MA equation,

log detD2φ = −V + V (∇φ)− cq + q(∇φ).

- Differentiating the left side twice in the e1-direction andevaluating at x0,

∂11(LHS) = − tr([

[D2φ]−1D2φ1

]2)+ tr

([D2φ]−1D2φ11

)≤ 0

- On the right side,

∂11(RHS) = −V11 + 〈∇V (∇φ),∇φ11〉+ 〈D2V (∇φ)∇φ1,∇φ1〉+ 〈∇q(∇φ),∇φ11〉+ 〈D2q(∇φ)∇φ1,∇φ1〉

≥ −Λ + (λ− λq)|∇φ1(x0)|2.

- Hence, if λ− λq > 0, then |∇φ1(x0)| ≤√

Λ/(λ− λq).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 8 / 16

Page 14: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since our potential φ solves a MA equation,

log detD2φ = −V + V (∇φ)− cq + q(∇φ).

- Differentiating the left side twice in the e1-direction andevaluating at x0,

∂11(LHS) = − tr([

[D2φ]−1D2φ1

]2)+ tr

([D2φ]−1D2φ11

)≤ 0

- On the right side,

∂11(RHS) = −V11 + 〈∇V (∇φ),∇φ11〉+ 〈D2V (∇φ)∇φ1,∇φ1〉+ 〈∇q(∇φ),∇φ11〉+ 〈D2q(∇φ)∇φ1,∇φ1〉

≥ −Λ + (λ− λq)|∇φ1(x0)|2.

- Hence, if λ− λq > 0, then |∇φ1(x0)| ≤√

Λ/(λ− λq).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 8 / 16

Page 15: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since our potential φ solves a MA equation,

log detD2φ = −V + V (∇φ)− cq + q(∇φ).

- Differentiating the left side twice in the e1-direction andevaluating at x0,

∂11(LHS) = − tr([

[D2φ]−1D2φ1

]2)+ tr

([D2φ]−1D2φ11

)≤ 0

- On the right side,

∂11(RHS) = −V11 + 〈∇V (∇φ),∇φ11〉+ 〈D2V (∇φ)∇φ1,∇φ1〉+ 〈∇q(∇φ),∇φ11〉+ 〈D2q(∇φ)∇φ1,∇φ1〉

≥ −Λ + (λ− λq)|∇φ1(x0)|2.

- Hence, if λ− λq > 0, then |∇φ1(x0)| ≤√

Λ/(λ− λq).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 8 / 16

Page 16: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- Since our potential φ solves a MA equation,

log detD2φ = −V + V (∇φ)− cq + q(∇φ).

- Differentiating the left side twice in the e1-direction andevaluating at x0,

∂11(LHS) = − tr([

[D2φ]−1D2φ1

]2)+ tr

([D2φ]−1D2φ11

)≤ 0

- On the right side,

∂11(RHS) = −V11 + 〈∇V (∇φ),∇φ11〉+ 〈D2V (∇φ)∇φ1,∇φ1〉+ 〈∇q(∇φ),∇φ11〉+ 〈D2q(∇φ)∇φ1,∇φ1〉

≥ −Λ + (λ− λq)|∇φ1(x0)|2.

- Hence, if λ− λq > 0, then |∇φ1(x0)| ≤√

Λ/(λ− λq).

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 8 / 16

Page 17: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- If OT map takes x0 outside of BR , then the right side becomes,

∂11(RHS) = −V11 + 〈D2V (∇φ)∇φ1,∇φ1〉+ 0 + 0

≥ −Λ + λ|∇φ1(x0)|2.

- And so, |∇φ1(x0)| ≤√

Λ/λ.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 9 / 16

Page 18: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Some Heuristics

- If OT map takes x0 outside of BR , then the right side becomes,

∂11(RHS) = −V11 + 〈D2V (∇φ)∇φ1,∇φ1〉+ 0 + 0

≥ −Λ + λ|∇φ1(x0)|2.

- And so, |∇φ1(x0)| ≤√

Λ/λ.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 9 / 16

Page 19: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Where Does Our (Inverse) Transport Take Points?

- Question: Can we quantify how far points travel under our OT orits inverse?

- Answer: Yes.

Lemma

For any P ≥ R , there exists a constant P ′ = P ′(P , λ,Λ, λq) > 0 suchthat

T−1(BP) ⊆ BP′ .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 10 / 16

Page 20: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Where Does Our (Inverse) Transport Take Points?

- Question: Can we quantify how far points travel under our OT orits inverse?

- Answer: Yes.

Lemma

For any P ≥ R , there exists a constant P ′ = P ′(P , λ,Λ, λq) > 0 suchthat

T−1(BP) ⊆ BP′ .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 10 / 16

Page 21: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Where Does Our (Inverse) Transport Take Points?

- Question: Can we quantify how far points travel under our OT orits inverse?

- Answer: Yes.

Lemma

For any P ≥ R , there exists a constant P ′ = P ′(P , λ,Λ, λq) > 0 suchthat

T−1(BP) ⊆ BP′ .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 10 / 16

Page 22: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

A More Refined A Priori Estimate

Lemma

If h(x , α) := φαα(x)eψ(|∇φ(x)|) attains a maximum at some point(x0, α0) among all (x , α) ∈ Rn × Sn−1, then

h(x0, α0) ≤ C with C = C (R , λ,Λ, λq) > 0.

R P

ψ(t)

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 11 / 16

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A More Refined A Priori Estimate

Lemma

If h(x , α) := φαα(x)eψ(|∇φ(x)|) attains a maximum at some point(x0, α0) among all (x , α) ∈ Rn × Sn−1, then

h(x0, α0) ≤ C with C = C (R , λ,Λ, λq) > 0.

R P

ψ(t)

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 11 / 16

Page 24: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Two Cases

1: Our auxiliary function h attains a maximum at some point(x0, α0) ∈ Rn × Sn−1.

2: Our auxiliary function h is not guaranteed to achieve a maximumin Rn × Sn−1.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 12 / 16

Page 25: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Two Cases

1: Our auxiliary function h attains a maximum at some point(x0, α0) ∈ Rn × Sn−1.

2: Our auxiliary function h is not guaranteed to achieve a maximumin Rn × Sn−1.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 12 / 16

Page 26: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Two Cases

1: Our auxiliary function h attains a maximum at some point(x0, α0) ∈ Rn × Sn−1.

2: Our auxiliary function h is not guaranteed to achieve a maximumin Rn × Sn−1.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 12 / 16

Page 27: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Case 2

- First, we consider the approximating OT maps ∇φj = T j takinge−V to ecq,j−V

j+cq−q, where for j � R

V j(x) =

{V (x) x ∈ Bj(0)

+∞ x ∈ Bcj (0)

and cq,j > 0 are normalizing constants.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 13 / 16

Page 28: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Case 2

- Second, we use that the functions

hjε(x , α) := (φj(x + εα) + φj(x − εα)− 2φj(x))eψ(|∇φj (x)|)

achieve maxima outside BR for all ε� 1.

- Third, we formalize our original heuristics replacing pure secondderivatives with second order difference quotients to conclude thatφjαα ≤

√Λ/λ.

- Finally, we pass to the limit via stability of OT.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 14 / 16

Page 29: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Case 2

- Second, we use that the functions

hjε(x , α) := (φj(x + εα) + φj(x − εα)− 2φj(x))eψ(|∇φj (x)|)

achieve maxima outside BR for all ε� 1.

- Third, we formalize our original heuristics replacing pure secondderivatives with second order difference quotients to conclude thatφjαα ≤

√Λ/λ.

- Finally, we pass to the limit via stability of OT.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 14 / 16

Page 30: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Proof (Sketch) of Theorem: Case 2

- Second, we use that the functions

hjε(x , α) := (φj(x + εα) + φj(x − εα)− 2φj(x))eψ(|∇φj (x)|)

achieve maxima outside BR for all ε� 1.

- Third, we formalize our original heuristics replacing pure secondderivatives with second order difference quotients to conclude thatφjαα ≤

√Λ/λ.

- Finally, we pass to the limit via stability of OT.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 14 / 16

Page 31: Lipschitz Changes of Variables between Perturbations · PDF fileLipschitz Changes of Variables between Perturbations of Log-concave Measures Yash Jhaveri University of Texas at Austin

Other Theorems: 1-d and the Radially Symmetric Case

Theorem (Colombo, Figalli, -)

Let V : R→ R ∪ {∞} be a convex function and q be a boundedfunction such that e−V , e−V−q ∈ P(R). Then, the optimal transportT that takes e−V to e−V−q is Lipschitz and satisfies

‖ logT ′‖L∞(R) ≤ ‖q+‖L∞(R) + ‖q−‖L∞(R).

Theorem (Colombo, Figalli, -)

Let V : Rn → R ∪ {∞} be a convex, radially symmetric function andq be a bounded, radially symmetric function such thate−V , e−V−q ∈ P(Rn). Then, the optimal transport T that takes e−V

to e−V−q is Lipschitz: for a.e. x ∈ Rn

e−‖q+‖L∞(Rn)−‖q−‖L∞(Rn) Id ≤ ∇T (x) ≤ e‖q

+‖L∞(Rn)+‖q−‖L∞(Rn) Id .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 15 / 16

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Other Theorems: 1-d and the Radially Symmetric Case

Theorem (Colombo, Figalli, -)

Let V : R→ R ∪ {∞} be a convex function and q be a boundedfunction such that e−V , e−V−q ∈ P(R). Then, the optimal transportT that takes e−V to e−V−q is Lipschitz and satisfies

‖ logT ′‖L∞(R) ≤ ‖q+‖L∞(R) + ‖q−‖L∞(R).

Theorem (Colombo, Figalli, -)

Let V : Rn → R ∪ {∞} be a convex, radially symmetric function andq be a bounded, radially symmetric function such thate−V , e−V−q ∈ P(Rn). Then, the optimal transport T that takes e−V

to e−V−q is Lipschitz: for a.e. x ∈ Rn

e−‖q+‖L∞(Rn)−‖q−‖L∞(Rn) Id ≤ ∇T (x) ≤ e‖q

+‖L∞(Rn)+‖q−‖L∞(Rn) Id .

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 15 / 16

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The End

Thank you.

Yash Jhaveri (UT Austin) Lipschitz Changes of Variables September 25, 2015 16 / 16