The distortion coefficients σ_{K,N}^{(t)}(θ) and τ_{K,N}^{(t)}(θ) #
The curvature-dimension conditions CD(K, N) and CD*(K, N) of Sturm and Lott–Villani, and the
measure-contraction property MCP(K, N), compare the reference measure along a Wasserstein
geodesic with the model space of constant curvature K / N (or K / (N - 1)) through two families
of distortion coefficients. For a curvature bound K : ℝ, a dimension bound N, a time t and
a distance θ, put D = K θ² / N. Then
σ_{K,N}^{(t)}(θ) = ∞ifD ≥ π²,σ_{K,N}^{(t)}(θ) = sin (t √D) / sin √Dif0 < D < π²,σ_{K,N}^{(t)}(θ) = tifD = 0,σ_{K,N}^{(t)}(θ) = sinh (t √(-D)) / sinh √(-D)ifD < 0,
and, for N > 1, τ_{K,N}^{(t)}(θ) = ∞ if (N - 1) π² ≤ K θ² (exactly when
σ_{K,N-1}^{(t)}(θ) = ∞) and τ_{K,N}^{(t)}(θ) = t ^ (1 / N) σ_{K,N-1}^{(t)}(θ) ^ (1 - 1 / N)
otherwise, with τ_{K,1}^{(t)}(θ) = ∞ for K θ² > 0 and τ_{K,1}^{(t)}(θ) = t for K θ² ≤ 0.
This N = 1 case deviates from Sturm at distance zero: Sturm puts τ_{K,1}^{(t)}(θ) = ∞ for
every K > 0, including θ = 0, whereas here τ_{K,1}^{(t)}(0) = t, the limit of
τ_{K,N}^{(t)}(0) = t as N ↓ 1. The two conventions agree whenever θ ≠ 0 or K ≤ 0.
For 0 < D < π² and θ ≥ 0, √D = θ √(K / N), so the second case of σ is the familiar
sin (t θ √(K / N)) / sin (θ √(K / N)).
Both families take values in [0, ∞] for t ∈ [0, 1], so they are ℝ≥0∞-valued here. The value
∞ records the Bonnet–Myers phenomenon: under CD(K, N) with K > 0 no two points are at
distance more than π √((N - 1) / K). As in Sturm, the critical-distance case of τ is ∞
for every t, including t = 0, rather than the ℝ≥0∞ product 0 · ∞ = 0. Outside
t ∈ [0, 1], N > 0 for σ and N ≥ 1 for τ, the values are junk values carrying no meaning.
The basic theory is the dependence on the parameters. For t ∈ [0, 1] the coefficient
σ_{K,N}^{(t)}(θ) depends on (K, N, θ) only through D and is monotone in D
(TauCeti.distortionSigma_mono). This rests on the monotonicity of the model ratios
Real.monotoneOn_sin_mul_div_sin and Real.antitoneOn_sinh_mul_div_sinh, and on the comparisons
Real.mul_sin_le_sin_mul and Real.sinh_mul_le_mul_sinh with the flat value t. Hence both
coefficients increase with the curvature bound K. In particular they are at least t for
K ≥ 0 and at most t for K ≤ 0, with equality σ_{0,N}^{(t)}(θ) = τ_{0,N}^{(t)}(θ) = t in
the flat case. This monotonicity is what makes the curvature-dimension conditions weaker as K
decreases, as in the implication from CD(K, N) to CD(K', N) for K' ≤ K.
Main definitions #
TauCeti.distortionSigma K N t θ: the distortion coefficientσ_{K,N}^{(t)}(θ).TauCeti.distortionTau K N t θ: the distortion coefficientτ_{K,N}^{(t)}(θ).
Main statements #
TauCeti.distortionSigma_mono: fort ∈ [0, 1],σ_{K,N}^{(t)}(θ) ≤ σ_{K',N'}^{(t)}(θ')wheneverK θ² / N ≤ K' θ'² / N'.TauCeti.distortionSigma_left_monotone,TauCeti.distortionTau_left_monotone: both coefficients are monotone in the curvature boundK.TauCeti.antitoneOn_distortionSigma_of_nonneg,TauCeti.monotoneOn_distortionSigma_of_nonpos:σ_{K,N}decreases withNforK ≥ 0and increases withNforK ≤ 0.TauCeti.distortionSigma_zero_left,TauCeti.distortionTau_zero_left: the flat coefficients aret.TauCeti.ofReal_le_distortionSigma,TauCeti.distortionSigma_le_ofRealand theirτanalogues: comparison with the flat valuetforK ≥ 0and forK ≤ 0.TauCeti.distortionSigma_eq_top_iff,TauCeti.distortionTau_eq_top_iff: forN > 0,σ_{K,N}^{(t)}(θ)is infinite exactly whenN π² ≤ K θ²; forN > 1,τ_{K,N}^{(t)}(θ)is infinite exactly when(N - 1) π² ≤ K θ².TauCeti.distortionTau_eq_top_of_lt: forK > 0,τ_{K,N}^{(t)}(θ)is infinite beyond the Bonnet–Myers distanceπ √((N - 1) / K), andTauCeti.distortionSigma_eq_top_of_lt: forK > 0andN > 0,σ_{K,N}^{(t)}(θ)is infinite beyondπ √(N / K).TauCeti.distortionSigma_time_one,TauCeti.distortionTau_time_one: below the critical distance both coefficients equal1at time1.
References #
- K.-T. Sturm, On the geometry of metric measure spaces. II, Acta Math. 196 (2006), 133–177.
- K. Bacher and K.-T. Sturm, Localization and tensorization properties of the curvature-dimension condition for metric measure spaces, J. Funct. Anal. 259 (2010), 28–56.
- C. Villani, Optimal Transport: Old and New, Springer 2009, Chapters 14 and 29.
The distortion coefficient σ_{K,N}^{(t)}(θ) of the curvature-dimension condition
CD*(K, N). With D = K θ² / N, it is ∞ if π² ≤ D, sin (t √D) / sin √D if 0 < D < π²,
t if D = 0, and sinh (t √(-D)) / sinh √(-D) if D < 0. It is meaningful for N > 0 and
t ∈ [0, 1].
Instances For
The distortion coefficient τ_{K,N}^{(t)}(θ) of the curvature-dimension condition
CD(K, N). For N > 1 it is ∞ if (N - 1) π² ≤ K θ² and
t ^ (1 / N) σ_{K,N-1}^{(t)}(θ) ^ (1 - 1 / N) otherwise, while τ_{K,1}^{(t)}(θ) is ∞ for
K θ² > 0 and t for K θ² ≤ 0; unlike Sturm, who puts τ_{K,1}^{(t)}(θ) = ∞ for every
K > 0, this gives τ_{K,1}^{(t)}(0) = t, the limit of τ_{K,N}^{(t)}(0) as N ↓ 1. It is
meaningful for N ≥ 1 and t ∈ [0, 1].
Instances For
The coefficient σ #
The flat coefficient σ_{0,N}^{(t)}(θ) is t.
At distance 0 the coefficient σ_{K,N}^{(t)}(0) is t.
For t ∈ [0, 1] and N ≥ 0, σ_{K,N}^{(t)}(θ) is monotone in the curvature bound K.
For t ∈ [0, 1] and K ≥ 0, σ_{K,N}^{(t)}(θ) decreases with the dimension bound N > 0.
For t ∈ [0, 1] and K ≤ 0, σ_{K,N}^{(t)}(θ) increases with the dimension bound N > 0.
The coefficient τ #
For N = 1 and K θ² > 0, the coefficient τ_{K,1}^{(t)}(θ) is infinite.
For N = 1 and K θ² ≤ 0, the coefficient τ_{K,1}^{(t)}(θ) is t.
The flat coefficient τ_{0,N}^{(t)}(θ) is t.
At distance 0 the coefficient τ_{K,N}^{(t)}(0) is t.
For t ∈ [0, 1], τ_{K,N}^{(t)}(θ) is monotone in the curvature bound K.
For K ≥ 0 the coefficient τ_{K,N}^{(t)}(θ) is at least the flat value t.
For K ≤ 0 the coefficient τ_{K,N}^{(t)}(θ) is at most the flat value t.