The Aleksandrov Monge–Ampère measure of a convex function #
Let E be a finite-dimensional real inner product space with an additive Haar measure μ, and
let f : E → EReal be convex (convex real epigraph, never ⊥), with D the interior of its
effective domain {x | f x ≠ ⊤}. The subgradient image of a set s is
∂f(s) = ⋃ x ∈ s, ∂f(x) (TauCeti.subgradientImage), the union of the subdifferentials of f
for the inner product. The Aleksandrov Monge–Ampère measure of f is
MA_f(s) = μ(∂f(s ∩ D))
for Borel s. It gives the weak (Aleksandrov) sense in which a merely convex function solves
the Monge–Ampère equation det D²f = ν. The same formula defines a measure for every μ
absolutely continuous with respect to a Haar measure, such as the weighted measure
s ↦ ∫_{∂f(s ∩ D)} g for μ = volume.withDensity g.
That s ↦ μ(∂f(s ∩ D)) is a measure rests on two facts.
- A point
ythat is a subgradient at two distinct pointsx₁ ≠ x₂is a point where the conjugatef⋆has the two subgradientsx₁andx₂, sof⋆is not differentiable there. By Rademacher's theorem for the convex functionf⋆, such points form aμ-null set (TauCeti.measure_setOf_exists_ne_mem_subdifferential_eq_zero); this needs no convexity off. Hence the subgradient images of disjoint sets are almost disjoint. - The subgradient image of a compact subset of
Dis compact (TauCeti.isCompact_subgradientImage). Open subsets ofDare σ-compact, so their subgradient images are measurable; complements are handled by the almost-disjointness, so the subgradient image of every Borel subset ofDis null measurable (TauCeti.nullMeasurableSet_subgradientImage).
A finite convex function u on an open convex set Ω is covered by extending it by ⊤ off Ω;
then D = Ω and the subdifferential is the set of y with u x + ⟪x' - x, y⟫ ≤ u x' for all
x' ∈ Ω (TauCeti.mongeAmpereMeasure_ite_apply).
For a convex function that is twice differentiable on D, the Aleksandrov measure is the
classical one, MA_f = det (D²f) dx on D (TauCeti.mongeAmpereMeasure_eq_withDensity_det).
On D the subdifferential is the gradient, so MA_f(s) = μ(∇f(s ∩ D)). This is computed by the
change of variables formula along the gradient
(TauCeti.withDensity_image_gradient_eq_setLIntegral): on a set where the subdifferential is the
single gradient ∇f x and has a positive derivative H x, the gradient is injective where H x
is nondegenerate (TauCeti.apply_sub_eq_zero_of_forall_mem_subdifferential_norm_sub_le) and maps
the set where H x is degenerate to a null set. The Hessian of a convex function is positive
(TauCeti.isPositive_of_hasFDerivAt_gradient).
The Aleksandrov maximum principle bounds a convex function by its Monge–Ampère mass: if u is
convex on a bounded open convex Ω, continuous on the closure and nonnegative on the frontier,
then max (-u x₀) 0 ^ n ≤ C diam(Ω) ^ (n - 1) dist(x₀, ∂Ω) MA_u(Ω) for x₀ ∈ Ω, with
C = 2 ^ (n + 1) / μ (ball 0 1)
(TauCeti.ofReal_neg_pow_mul_addHaar_ball_le_mul_mongeAmpereMeasure). Every slope p of an
affine function through (x₀, u x₀) lying below u on the frontier is a subgradient of u at
some point of Ω (TauCeti.exists_forall_add_inner_le_of_forall_frontier). When u ≥ 0 on the
frontier and u x₀ < 0, these slopes include a convex set containing a ball of radius
-u x₀ / diam Ω and a point of norm -u x₀ / dist(x₀, ∂Ω), and the volume of such a set is
bounded below by Convex.ofReal_dist_mul_pow_mul_addHaar_ball_le.
Main definitions #
TauCeti.mongeAmpereMeasure μ f— the Aleksandrov Monge–Ampère measure off; it is0whenfis not convex orμis not absolutely continuous with respect to a Haar measure.
Main statements #
TauCeti.measure_setOf_exists_ne_mem_subdifferential_eq_zeroandTauCeti.aedisjoint_subgradientImage— almost no point is a subgradient at two distinct points, so subgradient images of disjoint sets are almost disjoint;TauCeti.mongeAmpereMeasure_apply—MA_f(s) = μ(∂f(s ∩ D))for measurables;TauCeti.mongeAmpereMeasure_add—MA_fis additive in the reference measure, among measures absolutely continuous with respect to an additive Haar measure;TauCeti.mongeAmpereMeasure_compl_interior—MA_fis concentrated onD;TauCeti.mongeAmpereMeasure_lt_topandTauCeti.isLocallyFiniteMeasure_comap_mongeAmpereMeasure— whenμis finite on compact sets,MA_fis finite on compact subsets ofD, so it is a locally finite measure onD;TauCeti.sigmaFinite_mongeAmpereMeasure— whenμis finite on compact sets,MA_fis σ-finite for everyf;TauCeti.mongeAmpereMeasure_ite_apply— the formula for a finite convex function on an open set;TauCeti.mongeAmpereMeasure_ite_eq_restrict— the measure is local: restricting a convex function to an open convex subset restricts its Monge–Ampère measure;TauCeti.withDensity_restrict_le_mongeAmpereMeasureandTauCeti.mongeAmpereMeasure_le_withDensity_restrict— comparison of a density with the Monge–Ampère measure on an open convex subset;TauCeti.injOn_gradient_inter_setOf_det_ne_zero— the gradient is injective on the points where the subdifferential is the single gradient with an expansion of nonzero determinant;TauCeti.withDensity_image_gradient_eq_setLIntegral— the change of variables formula∫_{∇F(t)} g dμ = ∫_t det (H x) g (∇F x) dμalong the gradient of a convex function, on a settwhere the subdifferential is the single gradient with positive derivativeH x;TauCeti.mongeAmpereMeasure_eq_withDensity_detandTauCeti.mongeAmpereMeasure_ite_eq_withDensity_det— for a twice differentiable convex function, the Aleksandrov measure isdet (D²f) dxon the interior of the effective domain;TauCeti.ofReal_neg_pow_mul_addHaar_ball_le_mul_mongeAmpereMeasure— the Aleksandrov maximum principle.
References #
- A. D. Aleksandrov, Dirichlet's problem for the equation Det ‖z_{ij}‖ = φ(z₁, …, zₙ, z, x₁, …, xₙ). I, Vestnik Leningrad. Univ. Ser. Mat. Meh. Astr. 13 (1958), 5–24.
- C. E. Gutiérrez, The Monge–Ampère Equation, 2nd ed., Progress in Nonlinear Differential Equations and Their Applications 89, Birkhäuser, 2016, §1.1, in particular Theorem 1.1.13, and §1.4 for the Aleksandrov maximum principle.
- A. Figalli, The Monge–Ampère Equation and Its Applications, Zurich Lectures in Advanced Mathematics, EMS, 2017, §2.1, in particular Theorem 2.3.
Almost no point is a subgradient at two distinct points. For any f : E → EReal on a
finite-dimensional real inner product space, the set of y lying in the subdifferentials of f
at two distinct points is null for every additive Haar measure.
Subgradient images of disjoint sets are almost disjoint. For any f : E → EReal on a
finite-dimensional real inner product space, the subgradient images of disjoint sets meet in a
null set for every additive Haar measure.
Subgradient images of Borel subsets of the domain are null measurable. For a convex
f : E → EReal on a finite-dimensional real inner product space, the subgradient image of the
part of a measurable set inside the interior of the effective domain is null measurable for every
additive Haar measure. If f takes the value ⊥, then no point has a subgradient and the image
is empty.
The Aleksandrov Monge–Ampère measure of f : E → EReal with respect to a measure μ
that is absolutely continuous with respect to an additive Haar measure. When f is convex
(convex real epigraph, never ⊥), it is the measure with MA_f(s) = μ(∂f(s ∩ D)) for
measurable s, where D is the interior of the effective domain and ∂f the subgradient image
for the inner product (mongeAmpereMeasure_apply). For an additive Haar μ this is the
Aleksandrov measure; for μ = ν.withDensity g it is the weighted measure ∫_{∂f(s ∩ D)} g dν.
If f is not convex, or μ is not absolutely continuous with respect to a Haar measure, it is
0.
Instances For
The Aleksandrov Monge–Ampère measure of a convex function evaluated on a measurable set s is
the measure of the subgradient image of the part of s in the interior of the effective domain.
The Aleksandrov Monge–Ampère measure of a function whose real epigraph is not convex is
0.
The Aleksandrov Monge–Ampère measure of a function taking the value ⊥ is 0.
The Aleksandrov Monge–Ampère measure with respect to a measure that is not absolutely
continuous with respect to an additive Haar measure is 0.
The Aleksandrov Monge–Ampère measure is additive in the reference measure, among measures absolutely continuous with respect to an additive Haar measure.
The Aleksandrov Monge–Ampère measure is concentrated on the interior of the effective domain.
The Aleksandrov Monge–Ampère measure of a convex function, with respect to a measure that is finite on compact sets, is finite on every compact subset of the interior of the effective domain.
The Aleksandrov Monge–Ampère measure of a convex function, with respect to a measure that is finite on compact sets, is a locally finite measure on the interior of the effective domain.
The Aleksandrov Monge–Ampère measure with respect to a measure that is finite on compact sets
is σ-finite. For a convex function it is carried by the interior of the effective domain, which is
a countable union of compact sets of finite Monge–Ampère measure; otherwise it is 0.
The Aleksandrov Monge–Ampère measure of a finite convex function on an open set. Let u
be convex on an open set Ω, extended by ⊤ off Ω. On a measurable set s, its Monge–Ampère
measure is the measure of the set of y that are subgradients of u relative to Ω at some
point of s ∩ Ω, i.e. satisfy u x + ⟪x' - x, y⟫ ≤ u x' for every x' ∈ Ω.
The Aleksandrov Monge–Ampère measure is local. Let u be convex on an open set Ω, and
let U ⊆ Ω be open and convex. The Monge–Ampère measure of u restricted to U (extended by ⊤
off U) is the restriction to U of the Monge–Ampère measure of u on Ω: a subgradient of u
relative to the neighbourhood U of a point is a subgradient relative to Ω.
Density below an Aleksandrov subsolution on an open convex set. Let u be convex on an open
set Ω and U ⊆ Ω open and convex. If f dμ ≤ MA_u^Ω on Ω, where MA_u^Ω is the
Monge–Ampère measure of u extended by ⊤ off Ω, then every density g ≤ f on U satisfies
g dμ ≤ MA_u^U on U, where MA_u^U is the Monge–Ampère measure of u extended by ⊤ off
U.
Density above an Aleksandrov supersolution on an open convex set. Let u be convex on an
open set Ω and U ⊆ Ω open and convex. If MA_u^Ω ≤ f dμ on Ω, where MA_u^Ω is the
Monge–Ampère measure of u extended by ⊤ off Ω, then every density g ≥ f on U satisfies
MA_u^U ≤ g dμ on U, where MA_u^U is the Monge–Ampère measure of u extended by ⊤ off
U.
Change of variables along the gradient #
The gradient of a convex f : E → EReal is injective on the points of a set t at which the
subdifferential of f is the single gradient ∇F x, with the expansion
y' = ∇F x + H x (x' - x) + o(‖x' - x‖), and det (H x) ≠ 0. If two such points x₁ ≠ x₂ had
the same gradient, it would be a subgradient along the segment between them, and the expansion
at x₁ would vanish in the direction x₂ - x₁
(apply_sub_eq_zero_of_forall_mem_subdifferential_norm_sub_le).
Change of variables along the gradient of a convex function. Let f : E → EReal be convex,
with real representative F x = (f x).toReal, and let t be a set at each point of
which the subdifferential of f is the single gradient ∇F x, with the expansion
y' = ∇F x + H x (x' - x) + o(‖x' - x‖) for a positive H x, and suppose the part of t where
det (H x) ≠ 0 is measurable. Then ∫_{∇F(t)} g dμ = ∫_t det (H x) g (∇F x) dμ for
every additive Haar measure μ. The gradient is injective on the nondegenerate part of t, by
apply_sub_eq_zero_of_forall_mem_subdifferential_norm_sub_le, and maps the degenerate part to a
null set.
The Monge–Ampère measure of a twice differentiable convex function is det (D²f) dx.
Let f : E → EReal be convex and never ⊥, with real representative F x = (f x).toReal, and
suppose that on the interior D of the effective domain both F and its gradient ∇ F are
differentiable. Then for every additive Haar measure μ, the Aleksandrov Monge–Ampère measure of
f is μ restricted to D with density det (D(∇ F)), the determinant of the Hessian.
The Monge–Ampère measure of a twice differentiable convex function on an open set. If u
is convex on an open set Ω, and u and its gradient are differentiable on Ω, then the
Aleksandrov Monge–Ampère measure of u (extended by ⊤ off Ω) is det (D²u) dx on Ω: it is
μ restricted to Ω with density det (D(∇ u)), for every additive Haar measure μ. This
applies in particular to every convex u of class C² on Ω.
The Aleksandrov maximum principle #
The Aleksandrov maximum principle. Let Ω be a bounded open convex subset of a real inner
product space E of finite dimension n ≥ 1, and let u be convex on Ω, continuous on its
closure, and nonnegative on its frontier. Then at every x₀ ∈ Ω,
max (-u x₀) 0 ^ n * μ (ball 0 1) ≤ 2 ^ (n + 1) * diam Ω ^ (n - 1) * dist(x₀, ∂Ω) * MA_u(Ω),
where dist(x₀, ∂Ω) is the distance from x₀ to the complement of Ω and MA_u is the
Aleksandrov Monge–Ampère measure of u (extended by ⊤ off Ω) with respect to the additive
Haar measure μ. When MA_u(Ω) is finite, this bounds the negative part max (-u x₀) 0 above
on Ω and shows that max (-u x₀) 0 = O(dist(x₀, ∂Ω) ^ (1 / n)) as x₀ approaches the
boundary.