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Proof of The Mollified Density Cost is Bounded, Lipschitz for the Wasserstein Distance, and Below the Density Cost

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The bounds are those of the cost of the mollified density. For the Lipschitz bound, both mollified densities are written as integrals against an optimal coupling, Tonelli's theorem reduces the L1L^1 distance to the translation estimate for the kernel, and Cauchy-Schwarz turns the mean displacement into the Wasserstein distance. The comparison applies the supporting line of the integrand at each point against the translated kernel weights and integrates with Tonelli's theorem.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied to the data named here. The field axioms and the rules for adding inequalities, for multiplying them by nonnegative or positive real numbers, and for handling absolute values, from Elementary Order Arithmetic in an Ordered Field, Elementary Arithmetic in an Ordered Field and Properties of the Absolute Value in an Ordered Field, are used without further mention. For μ∈P(Rd)\mu\in\mathcal{P}(\mathbb{R}^{d}) we write ηε∗μ\eta_{\varepsilon}*\mu for the mollified density of Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost. For a nonnegative integrable function on a measure space, its real integral equals its integral as a nonnegative measurable function, its positive part being the function itself and its negative part 00 (Integrable Function and the Lebesgue Integral); conversely a nonnegative measurable real function whose integral in [0,∞][0,\infty] is finite is integrable, by the criterion of Measure Spaces and the Lebesgue Integral: Standing Notation §integral. These two facts are used without further mention. The integrals of nonnegative measurable functions obey claim 1 of Linearity and Monotonicity of the Lebesgue Integral, and those of integrable functions obey claim 2 there.

Step 1 (Claim 1). Let μ∈P2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}). By The Mollified Density Cost of a Probability Measure with Finite Second Moment §cost, GΦ,ε(μ)=∫RdΦ∘(ηε∗μ) dλd\mathcal{G}_{\Phi,\varepsilon}(\mu)=\int_{\mathbb{R}^{d}}\Phi\circ(\eta_{\varepsilon}*\mu)\,d\lambda_{d}, and Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §cost gives 0≤GΦ,ε(μ)≤L0\le\mathcal{G}_{\Phi,\varepsilon}(\mu)\le L.

Step 2 (Claim 2). Let DD be as in claim 2, put K0=ε−1(2+2dd κdD)K_{0}=\varepsilon^{-1}(2+2^{d}d\,\kappa_{d}D), so that K=L K0K=L\,K_{0}, and let μ,ν∈P2(Rd)\mu,\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}). Write a=ηε∗μa=\eta_{\varepsilon}*\mu and b=ηε∗νb=\eta_{\varepsilon}*\nu.

(2a) Reduction to the densities. By Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §density and Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §cost, the functions aa, bb, Φ∘a\Phi\circ a and Φ∘b\Phi\circ b are Borel, nonnegative and integrable with respect to λd\lambda_{d}. For y∈Rdy\in\mathbb{R}^{d}, let α\alpha and β\beta be the smaller and the larger of a(y),b(y)a(y),b(y); the Lipschitz bound of Convex Lipschitz Integrands §integrand gives ∣Φ(a(y))−Φ(b(y))∣=Φ(β)−Φ(α)≤L(β−α)=L ∣a(y)−b(y)∣|\Phi(a(y))-\Phi(b(y))|=\Phi(\beta)-\Phi(\alpha)\le L(\beta-\alpha)=L\,|a(y)-b(y)|. The functions Φ∘a−Φ∘b\Phi\circ a-\Phi\circ b and a−ba-b are integrable, their absolute values are measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions and have finite integrals, so they are integrable too; hence claim 2 of Linearity and Monotonicity of the Lebesgue Integral gives

∣GΦ,ε(μ)−GΦ,ε(ν)∣=∣∫Rd(Φ∘a−Φ∘b) dλd∣≤∫Rd∣Φ∘a−Φ∘b∣ dλd≤L∫Rd∣a−b∣ dλd.(1)\bigl|\mathcal{G}_{\Phi,\varepsilon}(\mu)-\mathcal{G}_{\Phi,\varepsilon}(\nu)\bigr|=\Bigl|\int_{\mathbb{R}^{d}}(\Phi\circ a-\Phi\circ b)\,d\lambda_{d}\Bigr|\le\int_{\mathbb{R}^{d}}|\Phi\circ a-\Phi\circ b|\,d\lambda_{d}\le L\int_{\mathbb{R}^{d}}|a-b|\,d\lambda_{d}.\tag{1}

(2b) An optimal coupling. By Existence of an Optimal Coupling of Two Probability Measures with Finite Second Moment (with m=dm=d) there is a coupling π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) whose quadratic cost satisfies I(π)=W2(μ,ν)2I(\pi)=W_{2}(\mu,\nu)^{2}. Its push-forwards by the coordinate projections pr1,pr2:Rd+d→Rd\mathrm{pr}_{1},\mathrm{pr}_{2}:\mathbb{R}^{d+d}\to\mathbb{R}^{d} of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs are μ\mu and ν\nu. Fix y∈Rdy\in\mathbb{R}^{d}. The function x↦ηε(y−x)x\mapsto\eta_{\varepsilon}(y-x) is Borel and integrable with respect to μ\mu and to ν\nu by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §density, so the change-of-variables formula of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pushforward gives that w↦ηε(y−pr1(w))w\mapsto\eta_{\varepsilon}(y-\mathrm{pr}_{1}(w)) and w↦ηε(y−pr2(w))w\mapsto\eta_{\varepsilon}(y-\mathrm{pr}_{2}(w)) are integrable with respect to π\pi, with

a(y)=∫Rd+dηε(y−pr1(w)) π(dw),b(y)=∫Rd+dηε(y−pr2(w)) π(dw).a(y)=\int_{\mathbb{R}^{d+d}}\eta_{\varepsilon}(y-\mathrm{pr}_{1}(w))\,\pi(dw),\qquad b(y)=\int_{\mathbb{R}^{d+d}}\eta_{\varepsilon}(y-\mathrm{pr}_{2}(w))\,\pi(dw).

Put F(w,y)=∣ηε(y−pr1(w))−ηε(y−pr2(w))∣F(w,y)=|\eta_{\varepsilon}(y-\mathrm{pr}_{1}(w))-\eta_{\varepsilon}(y-\mathrm{pr}_{2}(w))|. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral,

∣a(y)−b(y)∣≤∫Rd+dF(w,y) π(dw)for every y∈Rd.(2)|a(y)-b(y)|\le\int_{\mathbb{R}^{d+d}}F(w,y)\,\pi(dw)\qquad\text{for every }y\in\mathbb{R}^{d}.\tag{2}

(2c) Measurability. Write P1=pr1d+d,dP_{1}=\mathrm{pr}^{d+d,d}_{1} and P2=pr2d+d,dP_{2}=\mathrm{pr}^{d+d,d}_{2} for the coordinate projections of R(d+d)+d\mathbb{R}^{(d+d)+d} and ι′=ιd+d,d\iota'=\iota^{d+d,d} for the concatenation (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs). The maps pr1∘P1\mathrm{pr}_{1}\circ P_{1}, pr2∘P1\mathrm{pr}_{2}\circ P_{1} and P2P_{2} are Borel, as compositions of Borel maps (Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections, Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps); so by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §kernel (with m=(d+d)+dm=(d+d)+d) and claims 2 and 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, the function F^(v)=∣ηε(P2(v)−pr1(P1(v)))−ηε(P2(v)−pr2(P1(v)))∣\hat F(v)=|\eta_{\varepsilon}(P_{2}(v)-\mathrm{pr}_{1}(P_{1}(v)))-\eta_{\varepsilon}(P_{2}(v)-\mathrm{pr}_{2}(P_{1}(v)))| is Borel on R(d+d)+d\mathbb{R}^{(d+d)+d}. By Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product, ι′\iota' is measurable with respect to B(Rd+d)⊗B(Rd)\mathcal{B}(\mathbb{R}^{d+d})\otimes\mathcal{B}(\mathbb{R}^{d}) and B(R(d+d)+d)\mathcal{B}(\mathbb{R}^{(d+d)+d}), so F=F^∘ι′F=\hat F\circ\iota', which holds by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections, is measurable with respect to the product σ\sigma-algebra by claim 4 of Borel Measurability and Bounded Integration on a Metric Space; it is nonnegative.

(2d) Tonelli. The measure π\pi is a probability measure and λd\lambda_{d} is σ\sigma-finite by Lebesgue Measure on Euclidean Space is Sigma-Finite §sigma-finite. The Tonelli statement of Tonelli and Fubini Theorems, applied to (Rd+d,B(Rd+d),π)(\mathbb{R}^{d+d},\mathcal{B}(\mathbb{R}^{d+d}),\pi), (Rd,B(Rd),λd)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\lambda_{d}) and FF, shows that y↦∫F(w,y) π(dw)y\mapsto\int F(w,y)\,\pi(dw) is Borel and that

∫Rd(∫Rd+dF(w,y) π(dw))λd(dy)=∫Rd+d(∫RdF(w,y) λd(dy))π(dw)in [0,∞].\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d+d}}F(w,y)\,\pi(dw)\Bigr)\lambda_{d}(dy)=\int_{\mathbb{R}^{d+d}}\Bigl(\int_{\mathbb{R}^{d}}F(w,y)\,\lambda_{d}(dy)\Bigr)\pi(dw)\qquad\text{in }[0,\infty].

For each ww, Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §translation with x=pr1(w)x=\mathrm{pr}_{1}(w) and x′=pr2(w)x'=\mathrm{pr}_{2}(w) gives ∫F(w,y) λd(dy)≤K0 X(w)\int F(w,y)\,\lambda_{d}(dy)\le K_{0}\,X(w), where X(w)=∥pr1(w)−pr2(w)∥X(w)=\lVert\mathrm{pr}_{1}(w)-\mathrm{pr}_{2}(w)\rVert is Borel by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §functions. Combining with (2), by monotonicity,

∫Rd∣a−b∣ dλd≤∫Rd(∫Rd+dF(w,y) π(dw))λd(dy)≤K0∫Rd+dX dπ.(3)\int_{\mathbb{R}^{d}}|a-b|\,d\lambda_{d}\le\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d+d}}F(w,y)\,\pi(dw)\Bigr)\lambda_{d}(dy)\le K_{0}\int_{\mathbb{R}^{d+d}}X\,d\pi .\tag{3}

(2e) Cauchy-Schwarz. Since π(Rd+d)=1\pi(\mathbb{R}^{d+d})=1, (Rd+d,B(Rd+d),π)(\mathbb{R}^{d+d},\mathcal{B}(\mathbb{R}^{d+d}),\pi) is a probability space, on which XX and the constant Y=1Y=1 are random variables (claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions for YY). Pointwise X2=∥pr1−pr2∥2X^{2}=\lVert\mathrm{pr}_{1}-\mathrm{pr}_{2}\rVert^{2}, so E[X2]=I(π)=W2(μ,ν)2<∞\mathbb{E}[X^{2}]=I(\pi)=W_{2}(\mu,\nu)^{2}<\infty, and E[Y2]=π(Rd+d)=1\mathbb{E}[Y^{2}]=\pi(\mathbb{R}^{d+d})=1 by The Integral of an Indicator Function is the Measure of the Set, with expectations as in Expectation, Variance, and Moments. Hence XX and YY are square-integrable, with ∥X∥2=W2(μ,ν)\lVert X\rVert_{2}=W_{2}(\mu,\nu) and ∥Y∥2=1\lVert Y\rVert_{2}=1 by the uniqueness in Existence and Uniqueness of the Nonnegative Square Root, since W2(μ,ν)≥0W_{2}(\mu,\nu)\ge0 and 1≥01\ge0. As XY=XXY=X is nonnegative and integrable (Square-Integrable Random Variables and the Mean-Square Inner Product), claim 1 of Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm gives

∫Rd+dX dπ=E[XY]≤∥X∥2 ∥Y∥2=W2(μ,ν).\int_{\mathbb{R}^{d+d}}X\,d\pi=\mathbb{E}[XY]\le\lVert X\rVert_{2}\,\lVert Y\rVert_{2}=W_{2}(\mu,\nu).

With (1) and (3), ∣GΦ,ε(μ)−GΦ,ε(ν)∣≤L K0 W2(μ,ν)=K W2(μ,ν)|\mathcal{G}_{\Phi,\varepsilon}(\mu)-\mathcal{G}_{\Phi,\varepsilon}(\nu)|\le L\,K_{0}\,W_{2}(\mu,\nu)=K\,W_{2}(\mu,\nu). In the terms of Lipschitz Map Between Metric Spaces, with the metric W2W_{2} of The Quadratic Wasserstein Distance is a Metric on the Wasserstein Space §metric and the absolute-value metric, this is the Lipschitz property with constant KK. This proves claim 2.

Step 3 (Claim 3). Let μ∈P2ac(Rd)\mu\in\mathcal{P}_{2}^{\mathrm{ac}}(\mathbb{R}^{d}) and put a=ηε∗μa=\eta_{\varepsilon}*\mu. As recorded in The Density Cost of a Convex Lipschitz Integrand §cost, μ\mu has a density ρ\rho with respect to λd\lambda_{d} in the sense of The Radon-Nikodym Theorem for a Finite Measure and a Sigma-Finite Measure, and Uniqueness of Densities: ρ:Rd→R\rho:\mathbb{R}^{d}\to\mathbb{R} is Borel, ρ≥0\rho\ge0, and μ(A)=∫1Aρ dλd\mu(A)=\int\mathbf{1}_{A}\rho\,d\lambda_{d} for every A∈B(Rd)A\in\mathcal{B}(\mathbb{R}^{d}); moreover GΦ(μ)=∫RdΦ∘ρ dλd\mathcal{G}_{\Phi}(\mu)=\int_{\mathbb{R}^{d}}\Phi\circ\rho\,d\lambda_{d}. Thus μ\mu is the measure with density ρ\rho with respect to λd\lambda_{d} of claim 3 of Image Measures, Measures with Densities, and Change of Variables, and that claim gives

∫Rdf dμ=∫Rdf ρ dλdin [0,∞]for every Borel f:Rd→[0,∞].(4)\int_{\mathbb{R}^{d}}f\,d\mu=\int_{\mathbb{R}^{d}}f\,\rho\,d\lambda_{d}\quad\text{in }[0,\infty]\qquad\text{for every Borel }f:\mathbb{R}^{d}\to[0,\infty].\tag{4}

By Supporting Lines, Composition and Jensen's Inequality for a Convex Lipschitz Integrand §composition, applied to (Rd,B(Rd),λd)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\lambda_{d}) and h=ρh=\rho, the function Φ∘ρ\Phi\circ\rho is Borel and 0≤Φ(ρ(x))≤L ρ(x)0\le\Phi(\rho(x))\le L\,\rho(x) for every xx.

(3a) A pointwise inequality. Fix y∈Rdy\in\mathbb{R}^{d} and write ey(x)=ηε(y−x)e_{y}(x)=\eta_{\varepsilon}(y-x); by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §kernel (with m=dm=d, vv constant equal to yy and uu the identity) eye_{y} is Borel, and it is nonnegative. By Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §density, t0=a(y)t_{0}=a(y) lies in [0,∞)[0,\infty), and by (4) with f=eyf=e_{y} the nonnegative Borel function eyρe_{y}\rho (claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions) has integral t0t_{0} with respect to λd\lambda_{d}, so it is integrable with real integral t0t_{0}. By Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §kernel, ηε\eta_{\varepsilon} is a nonnegative Borel mollifier kernel, so by condition 4 of Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n it is integrable with integral 11; claim 2 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n, applied with n=dn=d, a=ya=y and f=ηεf=\eta_{\varepsilon}, gives ∫ey dλd=∫ηε(y−x) λd(dx)=∫ηε dλd=1\int e_{y}\,d\lambda_{d}=\int\eta_{\varepsilon}(y-x)\,\lambda_{d}(dx)=\int\eta_{\varepsilon}\,d\lambda_{d}=1, so eye_{y} is integrable with integral 11. By Supporting Lines, Composition and Jensen's Inequality for a Convex Lipschitz Integrand §support choose a real ss with Φ(t)≥Φ(t0)+s(t−t0)\Phi(t)\ge\Phi(t_{0})+s(t-t_{0}) for all t∈[0,∞)t\in[0,\infty). Taking t=ρ(x)t=\rho(x) and multiplying by ey(x)≥0e_{y}(x)\ge0,

ey(x) Φ(ρ(x))≥(Φ(t0)−s t0)ey(x)+s ey(x)ρ(x)(x∈Rd).e_{y}(x)\,\Phi(\rho(x))\ge\bigl(\Phi(t_{0})-s\,t_{0}\bigr)e_{y}(x)+s\,e_{y}(x)\rho(x)\qquad(x\in\mathbb{R}^{d}).

The right side is integrable with integral (Φ(t0)−s t0)⋅1+s t0=Φ(t0)(\Phi(t_{0})-s\,t_{0})\cdot1+s\,t_{0}=\Phi(t_{0}) by claim 2 of Linearity and Monotonicity of the Lebesgue Integral. The left side qy=ey⋅(Φ∘ρ)q_{y}=e_{y}\cdot(\Phi\circ\rho) is Borel (claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions) with 0≤qy≤L eyρ0\le q_{y}\le L\,e_{y}\rho, so its integral is at most L t0<∞L\,t_{0}<\infty and it is integrable. The monotonicity in claim 2 of Linearity and Monotonicity of the Lebesgue Integral gives

Φ(a(y))≤∫Rdηε(y−x) Φ(ρ(x)) λd(dx)for every y∈Rd.(5)\Phi(a(y))\le\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(y-x)\,\Phi(\rho(x))\,\lambda_{d}(dx)\qquad\text{for every }y\in\mathbb{R}^{d}.\tag{5}

(3b) Integration in yy. Let Q^(w)=ηε(pr2(w)−pr1(w)) Φ(ρ(pr1(w)))\hat{Q}(w)=\eta_{\varepsilon}(\mathrm{pr}_{2}(w)-\mathrm{pr}_{1}(w))\,\Phi(\rho(\mathrm{pr}_{1}(w))) for w∈Rd+dw\in\mathbb{R}^{d+d}; it is Borel by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §kernel (with m=d+dm=d+d, u=pr1u=\mathrm{pr}_{1}, v=pr2v=\mathrm{pr}_{2}), by composition (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps) and by claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and nonnegative. As in (2c), Q=Q^∘ιQ=\hat{Q}\circ\iota with the concatenation ι=ιd,d\iota=\iota^{d,d} is measurable with respect to B(Rd)⊗B(Rd)\mathcal{B}(\mathbb{R}^{d})\otimes\mathcal{B}(\mathbb{R}^{d}), and Q(x,y)=ηε(y−x)Φ(ρ(x))Q(x,y)=\eta_{\varepsilon}(y-x)\Phi(\rho(x)). The Tonelli statement of Tonelli and Fubini Theorems for (Rd,B(Rd),λd)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\lambda_{d}) twice and QQ gives

∫Rd(∫RdQ(x,y) λd(dx))λd(dy)=∫Rd(∫RdQ(x,y) λd(dy))λd(dx)in [0,∞].\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d}}Q(x,y)\,\lambda_{d}(dx)\Bigr)\lambda_{d}(dy)=\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d}}Q(x,y)\,\lambda_{d}(dy)\Bigr)\lambda_{d}(dx)\qquad\text{in }[0,\infty].

For each xx, by the multiple rule in claim 1 of Linearity and Monotonicity of the Lebesgue Integral with the constant Φ(ρ(x))≥0\Phi(\rho(x))\ge0 and by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §kernel, the inner integral on the right is Φ(ρ(x))∫ηε(y−x) λd(dy)=Φ(ρ(x))\Phi(\rho(x))\int\eta_{\varepsilon}(y-x)\,\lambda_{d}(dy)=\Phi(\rho(x)); so the right side is ∫Φ∘ρ dλd=GΦ(μ)\int\Phi\circ\rho\,d\lambda_{d}=\mathcal{G}_{\Phi}(\mu). By (5) and monotonicity, the left side is at least ∫RdΦ∘a dλd=GΦ,ε(μ)\int_{\mathbb{R}^{d}}\Phi\circ a\,d\lambda_{d}=\mathcal{G}_{\Phi,\varepsilon}(\mu), the function Φ∘a\Phi\circ a being nonnegative, Borel and integrable by Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost §cost. Hence GΦ,ε(μ)≤GΦ(μ)\mathcal{G}_{\Phi,\varepsilon}(\mu)\le\mathcal{G}_{\Phi}(\mu), which is claim 3.

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