The measure-contraction property MCP(K, N) #
Let M be a metric-measure space (TauCeti.MetricMeasureSpace): a complete separable metric
space X with its Borel structure and a reference measure m finite on bounded sets. For a
curvature bound K : ℝ and a dimension bound N : ℝ, M has the measure-contraction property
MCP(K, N) of Ohta and Sturm when the reference measure contracts towards every point of its
support at least as fast as in the model space of curvature K / (N - 1) and dimension N.
In the form of Cavalletti–Mondino used here: for every o in the support of m and every
measurable A with 0 < m(A) < ∞, the normalised restriction m[|A] = m(A)⁻¹ m|_A is joined to
the Dirac mass δ_o by a dynamic plan η concentrated on geodesics such that, for every time
t ∈ [0, 1],
(e_t)_# (τ_{K,N}^{(1-t)}(d(γ₀, γ₁))^N η(dγ)) ≤ m(A)⁻¹ m,
where e_t evaluates a path at time t and τ_{K,N} is the distortion coefficient
TauCeti.distortionTau. In words: the mass of A, transported along geodesics to o and
weighted by the distortion coefficient, never piles up above the reference measure. Since the
target is a Dirac mass, the only coupling of m[|A] and δ_o is their product, so every
dynamic plan concentrated on geodesics with these two time marginals is an optimal one; no
separate optimality requirement is needed. Ohta states the condition with the time reversed,
starting from δ_o at time 0; the two forms agree after reversing the paths.
The coefficient τ_{K,N}^{(s)}(θ) is infinite for K > 0 and θ beyond the Bonnet–Myers
distance π √((N - 1) / K), at every time s, following Sturm. With this convention the
condition at time t = 0 already forces the Bonnet–Myers diameter bound: under MCP(K, N)
with K > 0 and N > 0, any two points of the support of m are at distance at most
π √((N - 1) / K) (TauCeti.MetricMeasureSpace.MeasureContraction.dist_le).
On a finite-dimensional real normed space E of dimension n ≥ 1 with an additive Haar measure,
the plan moving m[|A] along straight segments to o shows that MCP(K, N) holds for every
K ≤ 0 and N ≥ n; conversely the time marginals of any plan from the unit ball to 0 are
carried by smaller balls, so MCP(0, N) forces N ≥ n. Thus Haar measure on E satisfies
MCP(0, N) exactly when N ≥ n
(TauCeti.MetricMeasureSpace.measureContraction_zero_iff_finrank_le), and MCP(K, N) for no
K > 0 and N > 0, its support being unbounded.
Main definitions #
TauCeti.MetricMeasureSpace.MeasureContraction M K N: the measure-contraction propertyMCP(K, N)of the metric-measure spaceM.
Main statements #
TauCeti.MetricMeasureSpace.MeasureContraction.mono: forN ≥ 0,MCP(K, N)impliesMCP(K', N)wheneverK' ≤ K.TauCeti.MetricMeasureSpace.MeasureContraction.dist_le,TauCeti.MetricMeasureSpace.MeasureContraction.diam_support_le: the Bonnet–Myers diameter bounddiam (supp m) ≤ π √((N - 1) / K)underMCP(K, N)withK > 0andN > 0.TauCeti.MetricMeasureSpace.measureContraction_of_nonpos_of_finrank_le: Haar measure on a real vector space of dimensionn ≥ 1satisfiesMCP(K, N)forK ≤ 0andN ≥ n.TauCeti.MetricMeasureSpace.finrank_le_of_measureContraction_zero,TauCeti.MetricMeasureSpace.measureContraction_zero_iff_finrank_le: Haar measure on a real vector space of dimensionnsatisfiesMCP(0, N)only forN ≥ n, and, forn ≥ 1, exactly then.TauCeti.MetricMeasureSpace.not_measureContraction_of_pos: Haar measure on a nontrivial real vector space satisfiesMCP(K, N)for noK > 0andN > 0.
References #
- S. Ohta, On the measure contraction property of metric measure spaces, Comment. Math. Helv. 82 (2007), 805–828, Definition 2.1.
- K.-T. Sturm, On the geometry of metric measure spaces. II, Acta Math. 196 (2006), 133–177, §5.
- F. Cavalletti and A. Mondino, Optimal maps in essentially non-branching spaces, Commun. Contemp. Math. 19 (2017), 1750007, Definition 2.4.
The measure-contraction property MCP(K, N) of Ohta and Sturm, in the form of
Cavalletti–Mondino: for every point o of the support of the reference measure m and every
measurable A with 0 < m(A) < ∞, some dynamic plan η concentrated on geodesics has law
m[|A] = m(A)⁻¹ m|_A at time 0 and law δ_o at time 1, and for every time t the law at
time t of η weighted by τ_{K,N}^{(1-t)}(d(γ₀, γ₁))^N is at most m(A)⁻¹ m.
Such a plan is automatically optimal, since m[|A] and δ_o have only one coupling.
The property is meaningful for N ≥ 1: for 0 < N ≤ 1 and K > 0 the distortion coefficient
distortionTau is ⊤ at positive distances, so MCP(K, N) then only says that the support of the
reference measure has at most one point.
Instances For
The measure-contraction property MCP(K, N), unfolded.
MCP(K, N) implies MCP(K', N) for every K' ≤ K, when N ≥ 0: the distortion coefficient
increases with the curvature bound.
The Bonnet–Myers diameter bound under MCP(K, N). If M satisfies MCP(K, N) with
K > 0 and N > 0, any two points of the support of the reference measure are at distance at
most π √((N - 1) / K). For N ≤ 1 this bound is 0 (as √ of a nonpositive number is 0), so
the lemma then says that the support has at most one point.
The Bonnet–Myers diameter bound under MCP(K, N), for K > 0 and N > 0: the support of
the reference measure has diameter at most π √((N - 1) / K).
Under MCP(K, N) with K > 0 and N > 0, the support of the reference measure is bounded.
Haar measure satisfies MCP(K, N) for K ≤ 0 and N ≥ n. On a real vector space of
finite dimension n ≥ 1, an additive Haar reference measure satisfies MCP(K, N) for every
K ≤ 0 and N ≥ n. The plan moves m[|A] along straight segments to o; its law at time t
is the image of m[|A] under the homothety of ratio 1 - t towards o.
MCP(0, N) forces N ≥ n for Haar measure. If an additive Haar reference measure on a
real vector space of finite dimension n satisfies MCP(0, N), then N ≥ n. At time 1 / 2,
any plan from the closed unit ball to 0 has its law carried by the ball of radius 1 / 2, of
relative volume 2^(-n), while the weight is 2^(-N).
Haar measure satisfies MCP(0, N) exactly when N ≥ n. On a real vector space of finite
dimension n ≥ 1, an additive Haar reference measure satisfies MCP(0, N) if and only if
N ≥ n.
Haar measure on a nontrivial real vector space of finite dimension satisfies MCP(K, N) for
no K > 0 and N > 0: its support is the whole unbounded space, against the Bonnet–Myers
bound.