Volume of sections of solutions of the Monge–Ampère equation #
Let E be a real inner product space of finite dimension n ≥ 1 with an additive Haar measure
μ, and let v be convex on a bounded open set G, continuous on its closure. The Monge–Ampère
mass of v on G, the volume of G and the depth of v below its boundary values control
each other, with constants depending only on E and μ:
- if
v ≥ 0on the frontier ofG, then(max 0 (-v x₀)) ^ n ≤ C μ(G) MA_v(G)for everyx₀ ∈ G; - if
v ≤ 0on the frontier ofG,v ≥ -honGandMA_v ≥ λ μonG, thenλ μ(G)² ≤ C hⁿ.
So a convex function with λ ≤ MA_v ≤ Λ vanishing on the boundary of G has depth comparable
to μ(G) ^ (2 / n). Both bounds are affine invariant. They are proved for a domain normalized by
an affine equivalence T between the balls of radii r and 1 about 0
(TauCeti.exists_affineEquiv_ball_subset_image_subset_ball), and transferred back by the change
of variables MA_{v ∘ T⁻¹}(s) = |det L| MA_v(T⁻¹ '' s), where L is the linear part of T⁻¹
(TauCeti.mongeAmpereMeasure_comp_affineEquiv_apply), together with
μ(T⁻¹ '' s) = |det L| μ(s). In the normalized position the first bound is the Aleksandrov
maximum principle (TauCeti.ofReal_neg_pow_mul_addHaar_ball_le_mul_mongeAmpereMeasure), and the
second is the comparison principle (TauCeti.le_of_mongeAmpereMeasure_le_of_le_frontier) against
the quadratic y ↦ (a / 2) (‖y‖² - r²) whose Monge–Ampère measure is aⁿ μ
(TauCeti.mongeAmpereMeasure_ite_mul_norm_sq_add).
Applied to v = u - u x - ℓ (· - x) - h on a section S = {y ∈ Ω | u y < u x + ℓ (y - x) + h}
whose closure lies in the domain Ω of u, these give the volume estimates for sections: if
λ ≤ MA_u ≤ Λ on Ω and ℓ is a supporting slope at x, then λ μ(S)² ≤ C hⁿ and
hⁿ ≤ C Λ μ(S)², i.e. μ(S) is comparable to h ^ (n / 2). These estimates are the starting
point for the geometry of sections used in the regularity theory of the Monge–Ampère equation.
Main statements #
TauCeti.mongeAmpereMeasure_ite_mul_norm_sq_add— the Monge–Ampère measure ofy ↦ (a / 2) ‖y‖² + con an open convex set isaⁿ μ;TauCeti.mongeAmpereMeasure_ite_convexSection_add_linearMap— subtracting a plane fromuon a sectionSrestricts the Monge–Ampère measure ofutoS;TauCeti.exists_ofReal_neg_pow_le_mul_ofReal_mul_measure_mul_mongeAmpereMeasure— the depth bound(max 0 (-v x₀)) ^ n ≤ C d μ(G) MA_v(G)whendbounds the distance to the boundary in every normalized position;TauCeti.exists_ofReal_neg_pow_le_mul_measure_mul_mongeAmpereMeasure— the depth bound(max 0 (-v x₀)) ^ n ≤ C μ(G) MA_v(G);TauCeti.exists_mul_measure_sq_le_mul_ofReal_pow— the volume boundλ μ(G)² ≤ C hⁿ;TauCeti.exists_ofReal_pow_le_mul_measure_convexSection_mul_mongeAmpereMeasureandTauCeti.exists_mul_measure_convexSection_sq_le_mul_ofReal_pow— the corresponding lower and upper volume estimateshⁿ ≤ C μ(S) MA_u(S)andλ μ(S)² ≤ C hⁿfor sections.TauCeti.abs_sub_le_on_convexSection_of_smul_le_mongeAmpereMeasure_le_smul— a quantitative comparison on a section with a given zero-boundary reference.
References #
- L. A. Caffarelli, A localization property of viscosity solutions to the Monge–Ampère equation and their strict convexity, Ann. of Math. 131 (1990), 129–134.
- C. E. Gutiérrez, The Monge–Ampère Equation, 2nd ed., Progress in Nonlinear Differential Equations and Their Applications 89, Birkhäuser, 2016, §3.2.
- A. Figalli, The Monge–Ampère Equation and Its Applications, Zurich Lectures in Advanced Mathematics, EMS, 2017, Chapter 4.
The Monge–Ampère measure of a quadratic. For a ≥ 0, the function
y ↦ (a / 2) ‖y‖² + c on an open convex set U, extended by ⊤ off U, has Monge–Ampère
measure aⁿ μ on U with respect to an additive Haar measure μ, where n = finrank ℝ E: its
gradient is y ↦ a • y.
On a positive-dimensional space, a constant potential on an open convex set,
extended by ⊤ outside it, has zero Monge–Ampère measure.
Subtracting a plane on a section. Let u be convex on an open set Ω, and let
S = {y ∈ Ω | u y < u x + ℓ (y - x) + h}. The Monge–Ampère measure of u + L + c, extended by
⊤ off S, is the restriction to S of the Monge–Ampère measure of u extended by ⊤ off
Ω. With L = -ℓ and c = ℓ x - u x - h this is the potential u - u x - ℓ (· - x) - h, which
vanishes on the frontier of S.
A lower bound a μ ≤ MA_u on Ω gives the lower bound a μ ≤ MA_{u + L + c} on a section
S of u, for the Monge–Ampère measures of u extended by ⊤ off Ω and of u + L + c
extended by ⊤ off S.
Quantitative comparison on a section. Subtract the defining plane and height of a
bounded section whose closure is in the original open domain. If the Monge–Ampère measure
restricted to that section lies between (1 - ε)^n • ν and (1 + ε)^n • ν, the resulting
zero-boundary potential differs from a zero-boundary reference v with measure ν by at
most ε |v| on the section.
The depth of a convex function is controlled by its distance to the boundary, volume and
Monge–Ampère mass. There is a constant C, depending only on E and μ, with the following
property. Let G be a bounded open set, v convex on G, continuous on its closure and
nonnegative on its frontier, and x₀ ∈ G. If d bounds the distance from T x₀ to the
complement of T '' G for every affine equivalence T mapping G into the unit ball, then
(max 0 (-v x₀)) ^ n ≤ C d μ(G) MA_v(G) for the Monge–Ampère measure of v extended by ⊤ off
G, where n = finrank ℝ E. Both the hypothesis and the conclusion are invariant under affine
changes of coordinates.
The depth of a convex function is controlled by its volume and Monge–Ampère mass. There
is a constant C, depending only on E and μ, such that for every bounded open set G, every
v convex on G, continuous on its closure and nonnegative on its frontier, and every x₀ ∈ G,
(max 0 (-v x₀)) ^ n ≤ C μ(G) MA_v(G) for the Monge–Ampère measure of v extended by ⊤ off
G, where n = finrank ℝ E. Unlike the Aleksandrov maximum principle it involves no diameter
or distance, so it is invariant under affine changes of coordinates.
The volume of a domain is controlled by the depth of a convex function on it. There is a
constant C, depending only on E and μ, with the following property. Let G be a bounded
open set and v convex on G, continuous on its closure, with v ≤ 0 on the frontier of G and
v ≥ -h on G. If the Monge–Ampère measure of v (extended by ⊤ off G) is at least λ μ
on G, then λ μ(G)² ≤ C hⁿ, where n = finrank ℝ E.
Sections #
Lower volume estimate for sections. There is a constant C, depending only on E and
μ, with the following property. Let u be convex on an open set Ω, let x ∈ Ω, and let
S = {y ∈ Ω | u y < u x + ℓ (y - x) + h} be a bounded section whose closure lies in Ω. Then
hⁿ ≤ C μ(S) MA_u(S) for the Monge–Ampère measure of u extended by ⊤ off Ω, where
n = finrank ℝ E. In particular, if MA_u ≤ Λ μ on Ω, then hⁿ ≤ C Λ μ(S)².
Upper volume estimate for sections. There is a constant C, depending only on E and
μ, with the following property. Let u be convex on an open set Ω, let ℓ be a supporting
slope of u at x, and let S = {y ∈ Ω | u y < u x + ℓ (y - x) + h} be a bounded section whose
closure lies in Ω. If the Monge–Ampère measure of u (extended by ⊤ off Ω) is at least
λ μ on Ω, then λ μ(S)² ≤ C hⁿ, where n = finrank ℝ E.