TheoremBase

The potential is the infimum over finite chains through the set of the Rockafellar-type chain sums for the halved squared torus distance: cyclical monotonicity bounds it below, chain extension gives the comparison inequality, the nearest-lift representation of the torus distance exhibits the convex lift as a supremum of affine functions, and the comparison inequality with a nearest lift gives the subgradient inequality.

Proof

Each result cited below is universally quantified over the data in its own statement. Throughout, L=d/2L=\sqrt{d}/2, a nonnegative real number, and for x,y∈Rdx,y\in\mathbb{R}^{d} we write

κ(x,y)=12 dT(x,y)2.\kappa(x,y)=\tfrac12\,d_{\mathbb{T}}(x,y)^{2}.

Finite sums ∑i=1m\sum_{i=1}^{m} are those of Finite Sum Notation in a Field in the field of real numbers; from Properties of Finite Sums we use the recursion and the independence of the extending family (claim 1), additivity (claim 2) and homogeneity (claim 3, with the factors 12\tfrac12 and −1-1, so that a finite sum of differences is the difference of the finite sums). Points of Rd\mathbb{R}^{d} are added, subtracted and scaled coordinatewise, as in Sum of Points of Rn\mathbb{R}^n, Scalar Multiple of a Point of Rn\mathbb{R}^n and Difference, Dot Product, and Orthogonality in Rn\mathbb{R}^n, and Rd\mathbb{R}^{d} is a real vector space by Euclidean Space Rn\mathbb{R}^n is a Real Vector Space. Since 0∈Z0\in\mathbb{Z} and Z\mathbb{Z} is closed under negation and addition (claim 2 of Arithmetic, Order, Discreteness and Intervals of the Integers), the lattice Zd\mathbb{Z}^{d} of Lattice-Periodic Functions and the Periodic Function Classes §lattice contains the origin 0Rd0_{\mathbb{R}^{d}} and is closed under negation and addition. The set Rd\mathbb{R}^{d} is convex, since every point t x+(1−t) yt\,x+(1-t)\,y with x,y∈Rdx,y\in\mathbb{R}^{d} lies in Rd\mathbb{R}^{d}.

Step 0. Three elementary facts.

(a) Expansion. For all a,b∈Rda,b\in\mathbb{R}^{d},

12∥a∥2−12∥a−b∥2=a⋅b−12∥b∥2.\tfrac12\lVert a\rVert^{2}-\tfrac12\lVert a-b\rVert^{2}=a\cdot b-\tfrac12\lVert b\rVert^{2}.

Indeed, by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n one has ∥a−b∥2=(a−b)⋅(a−b)\lVert a-b\rVert^{2}=(a-b)\cdot(a-b); by claims 3 and 5 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n this equals a⋅a−b⋅a−a⋅b+b⋅ba\cdot a-b\cdot a-a\cdot b+b\cdot b, and by claim 1 there (symmetry) together with claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n it equals ∥a∥2−2 a⋅b+∥b∥2\lVert a\rVert^{2}-2\,a\cdot b+\lVert b\rVert^{2}. Multiplying by 12\tfrac12 and subtracting from 12∥a∥2\tfrac12\lVert a\rVert^{2} gives the identity.

(b) Nearest lifts. Let x,y∈Rdx,y\in\mathbb{R}^{d}. For every y~∈y+Zd\tilde y\in y+\mathbb{Z}^{d},

dT(x,y)≤∥x−y~∥=∥y~−x∥and henceκ(x,y)≤12∥x−y~∥2;d_{\mathbb{T}}(x,y)\le\lVert x-\tilde y\rVert=\lVert\tilde y-x\rVert\qquad\text{and hence}\qquad\kappa(x,y)\le\tfrac12\lVert x-\tilde y\rVert^{2};

and the point y~x=x+ϖ(y−x)\tilde y_{x}=x+\varpi(y-x) belongs to y+Zdy+\mathbb{Z}^{d} and satisfies ∥x−y~x∥=dT(x,y)\lVert x-\tilde y_{x}\rVert=d_{\mathbb{T}}(x,y), hence κ(x,y)=12∥x−y~x∥2\kappa(x,y)=\tfrac12\lVert x-\tilde y_{x}\rVert^{2}. To see this, write y~=y+m\tilde y=y+m with m∈Zdm\in\mathbb{Z}^{d}. Then x−y~=(−1)(y−x−(−m))x-\tilde y=(-1)\bigl(y-x-(-m)\bigr) and y~−x=y−x−(−m)\tilde y-x=y-x-(-m), so claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n (with ∣−1∣=1|-1|=1) gives ∥x−y~∥=∥y~−x∥=∥y−x−(−m)∥\lVert x-\tilde y\rVert=\lVert\tilde y-x\rVert=\lVert y-x-(-m)\rVert; as −m∈Zd-m\in\mathbb{Z}^{d}, The Flat Torus Distance: Minimality of the Wrapped Displacement, Periodicity, the Metric on the Unit Cell and the Lipschitz Bound §minimal gives dT(x,y)≤∥y−x−(−m)∥d_{\mathbb{T}}(x,y)\le\lVert y-x-(-m)\rVert. Both dT(x,y)d_{\mathbb{T}}(x,y) (The Wrapped Displacement and the Flat Torus Distance §distance) and ∥x−y~∥\lVert x-\tilde y\rVert (claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n) are nonnegative, and for real numbers 0≤s≤t0\le s\le t one has s⋅s≤s⋅t≤t⋅ts\cdot s\le s\cdot t\le t\cdot t, multiplication by a nonnegative element preserving the order of the ordered field R\mathbb{R}; so dT(x,y)2≤∥x−y~∥2d_{\mathbb{T}}(x,y)^{2}\le\lVert x-\tilde y\rVert^{2}, and multiplying by 12\tfrac12 gives the second inequality. For y~x\tilde y_{x}: the point k0=y−x−ϖ(y−x)k_{0}=y-x-\varpi(y-x) lies in Zd\mathbb{Z}^{d} by The Flat Torus Distance: Minimality of the Wrapped Displacement, Periodicity, the Metric on the Unit Cell and the Lipschitz Bound §range, and y~x=y+(−k0)\tilde y_{x}=y+(-k_{0}) with −k0∈Zd-k_{0}\in\mathbb{Z}^{d}; moreover x−y~x=(−1)ϖ(y−x)x-\tilde y_{x}=(-1)\varpi(y-x), so ∥x−y~x∥=∥ϖ(y−x)∥=dT(x,y)\lVert x-\tilde y_{x}\rVert=\lVert\varpi(y-x)\rVert=d_{\mathbb{T}}(x,y) by claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and The Wrapped Displacement and the Flat Torus Distance §distance.

(c) Periodicity and Lipschitz bound of κ\kappa in the first variable. For all x,x′,y∈Rdx,x',y\in\mathbb{R}^{d} and k∈Zdk\in\mathbb{Z}^{d} one has κ(x+k,y)=κ(x,y)\kappa(x+k,y)=\kappa(x,y), by The Flat Torus Distance: Minimality of the Wrapped Displacement, Periodicity, the Metric on the Unit Cell and the Lipschitz Bound §symmetry applied with the lattice points kk and 0Rd0_{\mathbb{R}^{d}}; and ∣κ(x,y)−κ(x′,y)∣≤L∥x−x′∥|\kappa(x,y)-\kappa(x',y)|\le L\lVert x-x'\rVert, which is the second inequality of The Flat Torus Distance: Minimality of the Wrapped Displacement, Periodicity, the Metric on the Unit Cell and the Lipschitz Bound §lipschitz multiplied by 12\tfrac12.

Step 1. Chains and their values. Since Γ\Gamma is nonempty, fix once and for all a point w^∈Γ\hat w\in\Gamma and put x^=pr1(w^)\hat x=\mathrm{pr}_{1}(\hat w). A chain CC consists of a natural number NN with 2≤N2\le N and a map [N]→Γ[N]\to\Gamma, i↦wii\mapsto w_{i}, with w1=w^w_{1}=\hat w; we write xi=pr1(wi)x_{i}=\mathrm{pr}_{1}(w_{i}) and yi=pr2(wi)y_{i}=\mathrm{pr}_{2}(w_{i}) for i∈[N]i\in[N], so that x1=x^x_{1}=\hat x. Let C\mathcal{C} be the set of all chains; it is nonempty, containing the chain with N=2N=2 and w1=w2=w^w_{1}=w_{2}=\hat w. For a chain CC (with N−1∈NN-1\in\mathbb{N} because 2≤N2\le N) put

KC=∑i=1N−1(κ(xi+1,yi)−κ(xi,yi))−κ(xN,yN),gC(x)=KC+κ(x,yN)(x∈Rd).K_{C}=\sum_{i=1}^{N-1}\bigl(\kappa(x_{i+1},y_{i})-\kappa(x_{i},y_{i})\bigr)-\kappa(x_{N},y_{N}),\qquad g_{C}(x)=K_{C}+\kappa(x,y_{N})\quad(x\in\mathbb{R}^{d}).

These functions have the following four properties.

(i) 0≤gC(x^)0\le g_{C}(\hat x). Put xN+1=x1x_{N+1}=x_{1} and bi=κ(xi+1,yi)−κ(xi,yi)b_{i}=\kappa(x_{i+1},y_{i})-\kappa(x_{i},y_{i}) for i∈[N]i\in[N]. By the recursion of claim 1 of Properties of Finite Sums, applied with S(N−1)=NS(N-1)=N, and the independence of the extending family stated there,

∑i=1Nbi=∑i=1N−1(κ(xi+1,yi)−κ(xi,yi))+κ(x1,yN)−κ(xN,yN)=gC(x1)=gC(x^).\sum_{i=1}^{N}b_{i}=\sum_{i=1}^{N-1}\bigl(\kappa(x_{i+1},y_{i})-\kappa(x_{i},y_{i})\bigr)+\kappa(x_{1},y_{N})-\kappa(x_{N},y_{N})=g_{C}(x_{1})=g_{C}(\hat x).

By claims 2 and 3 of Properties of Finite Sums,

∑i=1Nbi=12(∑i=1NdT(xi+1,yi)2−∑i=1NdT(xi,yi)2),\sum_{i=1}^{N}b_{i}=\tfrac12\Bigl(\sum_{i=1}^{N}d_{\mathbb{T}}(x_{i+1},y_{i})^{2}-\sum_{i=1}^{N}d_{\mathbb{T}}(x_{i},y_{i})^{2}\Bigr),

which is nonnegative because Γ\Gamma is torus-cyclically monotone: that definition, applied to NN and the points w1,…,wN∈Γw_{1},\dots,w_{N}\in\Gamma, with xN+1=x1x_{N+1}=x_{1} exactly as there, gives ∑i=1NdT(xi,yi)2≤∑i=1NdT(xi+1,yi)2\sum_{i=1}^{N}d_{\mathbb{T}}(x_{i},y_{i})^{2}\le\sum_{i=1}^{N}d_{\mathbb{T}}(x_{i+1},y_{i})^{2}.

(ii) Periodicity. gC(x+k)=gC(x)g_{C}(x+k)=g_{C}(x) for all x∈Rdx\in\mathbb{R}^{d} and k∈Zdk\in\mathbb{Z}^{d}, by Step 0(c).

(iii) Lipschitz bound. ∣gC(x)−gC(x′)∣=∣κ(x,yN)−κ(x′,yN)∣≤L∥x−x′∥|g_{C}(x)-g_{C}(x')|=|\kappa(x,y_{N})-\kappa(x',y_{N})|\le L\lVert x-x'\rVert for all x,x′∈Rdx,x'\in\mathbb{R}^{d}, by Step 0(c).

(iv) Extension. Let w∈Γw\in\Gamma, x=pr1(w)x=\mathrm{pr}_{1}(w) and y=pr2(w)y=\mathrm{pr}_{2}(w), and let C+C^{+} be the chain with N+1N+1 points w1,…,wN,wN+1w_{1},\dots,w_{N},w_{N+1}, where wN+1=ww_{N+1}=w, so that xN+1=xx_{N+1}=x and yN+1=yy_{N+1}=y for C+C^{+}. The first N−1N-1 summands defining KC+K_{C^{+}} are those defining KCK_{C}, since they involve only w1,…,wNw_{1},\dots,w_{N}, and the recursion of claim 1 of Properties of Finite Sums, applied with S(N−1)=NS(N-1)=N, gives

KC+=∑i=1N−1(κ(xi+1,yi)−κ(xi,yi))+κ(x,yN)−κ(xN,yN)−κ(x,y)=gC(x)−κ(x,y).K_{C^{+}}=\sum_{i=1}^{N-1}\bigl(\kappa(x_{i+1},y_{i})-\kappa(x_{i},y_{i})\bigr)+\kappa(x,y_{N})-\kappa(x_{N},y_{N})-\kappa(x,y)=g_{C}(x)-\kappa(x,y).

Hence gC+(x′)=gC(x)+κ(x′,y)−κ(x,y)g_{C^{+}}(x')=g_{C}(x)+\kappa(x',y)-\kappa(x,y) for every x′∈Rdx'\in\mathbb{R}^{d}.

Step 2. Definition of φ\varphi. For x∈Rdx\in\mathbb{R}^{d} let S(x)={gC(x):C∈C}S(x)=\{g_{C}(x):C\in\mathcal{C}\}, a nonempty subset of R\mathbb{R} because C\mathcal{C} is nonempty. For every chain CC, (iii) and (i) give

gC(x)≥gC(x^)−L∥x−x^∥≥−L∥x−x^∥,g_{C}(x)\ge g_{C}(\hat x)-L\lVert x-\hat x\rVert\ge-L\lVert x-\hat x\rVert ,

so S(x)S(x) is bounded below by −L∥x−x^∥-L\lVert x-\hat x\rVert, and by Existence of the Infimum of a Nonempty Subset of R\mathbb{R} Bounded Below it has a greatest lower bound in R\mathbb{R}. Define φ(x)=inf⁡S(x)\varphi(x)=\inf S(x), and ψ(x)=12∥x∥2−φ(x)\psi(x)=\tfrac12\lVert x\rVert^{2}-\varphi(x) as in the statement. By the definition of a greatest lower bound we shall use two facts: φ(x)≤gC(x)\varphi(x)\le g_{C}(x) for every chain CC; and every real lower bound of S(x)S(x) is at most φ(x)\varphi(x).

Step 3. Claim 1. Let x∈Rdx\in\mathbb{R}^{d} and k∈Zdk\in\mathbb{Z}^{d}. By (ii), S(x+k)=S(x)S(x+k)=S(x), so φ(x+k)=φ(x)\varphi(x+k)=\varphi(x) and φ\varphi is Zd\mathbb{Z}^{d}-periodic. Let x,x′∈Rdx,x'\in\mathbb{R}^{d}. For every chain CC, Step 2 and (iii) give φ(x)≤gC(x)≤gC(x′)+L∥x−x′∥\varphi(x)\le g_{C}(x)\le g_{C}(x')+L\lVert x-x'\rVert, so φ(x)−L∥x−x′∥\varphi(x)-L\lVert x-x'\rVert is a lower bound of S(x′)S(x') and therefore φ(x)−L∥x−x′∥≤φ(x′)\varphi(x)-L\lVert x-x'\rVert\le\varphi(x'). Exchanging xx and x′x', and using ∥x′−x∥=∥x−x′∥\lVert x'-x\rVert=\lVert x-x'\rVert (claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n), we get ∣φ(x)−φ(x′)∣≤L∥x−x′∥|\varphi(x)-\varphi(x')|\le L\lVert x-x'\rVert. As ∥x−x′∥=dE(x,x′)\lVert x-x'\rVert=d_{E}(x,x') by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and ∣φ(x)−φ(x′)∣|\varphi(x)-\varphi(x')| is the distance of the absolute-value metric, φ\varphi is Lipschitz with constant L=d/2L=\sqrt{d}/2.

Step 4. Claim 3. Let w∈Γw\in\Gamma, x=pr1(w)x=\mathrm{pr}_{1}(w), y=pr2(w)y=\mathrm{pr}_{2}(w) and x′∈Rdx'\in\mathbb{R}^{d}. For every chain CC, Step 2 applied at x′x' to the chain C+C^{+} of (iv) gives

φ(x′)≤gC+(x′)=gC(x)+κ(x′,y)−κ(x,y).\varphi(x')\le g_{C^{+}}(x')=g_{C}(x)+\kappa(x',y)-\kappa(x,y).

Hence φ(x′)−κ(x′,y)+κ(x,y)\varphi(x')-\kappa(x',y)+\kappa(x,y) is a lower bound of S(x)S(x), so it is at most φ(x)\varphi(x); rearranging,

φ(x′)≤φ(x)+12dT(x′,y)2−12dT(x,y)2.\varphi(x')\le\varphi(x)+\tfrac12d_{\mathbb{T}}(x',y)^{2}-\tfrac12d_{\mathbb{T}}(x,y)^{2}.

Step 5. Claim 2. For a chain CC, whose last point has second coordinate yNy_{N}, and for y~∈yN+Zd\tilde y\in y_{N}+\mathbb{Z}^{d}, let fC,y~:Rd→Rf_{C,\tilde y}:\mathbb{R}^{d}\to\mathbb{R} be given by

fC,y~(x)=y~⋅x+(−12∥y~∥2−KC).f_{C,\tilde y}(x)=\tilde y\cdot x+\Bigl(-\tfrac12\lVert\tilde y\rVert^{2}-K_{C}\Bigr).

By claim 1 of Affine Functions, Sums, Nonnegative Multiples and Pointwise Suprema of Convex Functions, applied to the convex set Rd\mathbb{R}^{d}, the point p=y~p=\tilde y and the constant −12∥y~∥2−KC-\tfrac12\lVert\tilde y\rVert^{2}-K_{C}, each fC,y~f_{C,\tilde y} is convex on Rd\mathbb{R}^{d}. Let F\mathcal{F} be the set of all these functions; it is nonempty, since C\mathcal{C} is nonempty and yN=yN+0Rd∈yN+Zdy_{N}=y_{N}+0_{\mathbb{R}^{d}}\in y_{N}+\mathbb{Z}^{d}. Fix x∈Rdx\in\mathbb{R}^{d}; we show that ψ(x)\psi(x) is the least upper bound of {f(x):f∈F}\{f(x):f\in\mathcal{F}\}.

Upper bound. Let CC be a chain and y~∈yN+Zd\tilde y\in y_{N}+\mathbb{Z}^{d}. By Step 0(b), κ(x,yN)≤12∥x−y~∥2\kappa(x,y_{N})\le\tfrac12\lVert x-\tilde y\rVert^{2}, so gC(x)≤KC+12∥x−y~∥2g_{C}(x)\le K_{C}+\tfrac12\lVert x-\tilde y\rVert^{2}. By Step 0(a) and the symmetry of the dot product (claim 1 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n), and then Step 2,

fC,y~(x)=12∥x∥2−12∥x−y~∥2−KC≤12∥x∥2−gC(x)≤12∥x∥2−φ(x)=ψ(x).f_{C,\tilde y}(x)=\tfrac12\lVert x\rVert^{2}-\tfrac12\lVert x-\tilde y\rVert^{2}-K_{C}\le\tfrac12\lVert x\rVert^{2}-g_{C}(x)\le\tfrac12\lVert x\rVert^{2}-\varphi(x)=\psi(x).

Least. Let b∈Rb\in\mathbb{R} be an upper bound of {f(x):f∈F}\{f(x):f\in\mathcal{F}\}, and let CC be a chain. The point y~x=x+ϖ(yN−x)\tilde y_{x}=x+\varpi(y_{N}-x) of Step 0(b) lies in yN+Zdy_{N}+\mathbb{Z}^{d} and satisfies κ(x,yN)=12∥x−y~x∥2\kappa(x,y_{N})=\tfrac12\lVert x-\tilde y_{x}\rVert^{2}, so gC(x)=KC+12∥x−y~x∥2g_{C}(x)=K_{C}+\tfrac12\lVert x-\tilde y_{x}\rVert^{2} and, by the same identity as above, fC,y~x(x)=12∥x∥2−gC(x)f_{C,\tilde y_{x}}(x)=\tfrac12\lVert x\rVert^{2}-g_{C}(x). Hence 12∥x∥2−gC(x)≤b\tfrac12\lVert x\rVert^{2}-g_{C}(x)\le b, that is 12∥x∥2−b≤gC(x)\tfrac12\lVert x\rVert^{2}-b\le g_{C}(x). As CC was arbitrary, 12∥x∥2−b\tfrac12\lVert x\rVert^{2}-b is a lower bound of S(x)S(x), so 12∥x∥2−b≤φ(x)\tfrac12\lVert x\rVert^{2}-b\le\varphi(x), that is ψ(x)≤b\psi(x)\le b.

Thus for every xx the set {f(x):f∈F}\{f(x):f\in\mathcal{F}\} has an upper bound, and its least upper bound is ψ(x)\psi(x). Claim 4 of Affine Functions, Sums, Nonnegative Multiples and Pointwise Suprema of Convex Functions, applied to the convex set Rd\mathbb{R}^{d} and the nonempty family F\mathcal{F} of convex functions, shows that the function whose value at xx is that least upper bound, namely ψ\psi, is convex on Rd\mathbb{R}^{d}.

Step 6. Claim 4. Let w∈Γw\in\Gamma, x=pr1(w)x=\mathrm{pr}_{1}(w), y=pr2(w)y=\mathrm{pr}_{2}(w), and let y~∈y+Zd\tilde y\in y+\mathbb{Z}^{d} satisfy ∥y~−x∥=dT(x,y)\lVert\tilde y-x\rVert=d_{\mathbb{T}}(x,y). By claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, ∥x−y~∥=∥y~−x∥\lVert x-\tilde y\rVert=\lVert\tilde y-x\rVert, so κ(x,y)=12∥x−y~∥2\kappa(x,y)=\tfrac12\lVert x-\tilde y\rVert^{2}. Let x′∈Rdx'\in\mathbb{R}^{d}. By Step 0(b), κ(x′,y)≤12∥x′−y~∥2\kappa(x',y)\le\tfrac12\lVert x'-\tilde y\rVert^{2}, so claim 3 (Step 4) gives

φ(x′)≤φ(x)+12∥x′−y~∥2−12∥x−y~∥2,\varphi(x')\le\varphi(x)+\tfrac12\lVert x'-\tilde y\rVert^{2}-\tfrac12\lVert x-\tilde y\rVert^{2},

and therefore

ψ(x′)=12∥x′∥2−φ(x′)≥(12∥x′∥2−12∥x′−y~∥2)−φ(x)+12∥x−y~∥2.\psi(x')=\tfrac12\lVert x'\rVert^{2}-\varphi(x')\ge\Bigl(\tfrac12\lVert x'\rVert^{2}-\tfrac12\lVert x'-\tilde y\rVert^{2}\Bigr)-\varphi(x)+\tfrac12\lVert x-\tilde y\rVert^{2}.

By Step 0(a) with a=x′a=x' and b=y~b=\tilde y, the bracket equals x′⋅y~−12∥y~∥2x'\cdot\tilde y-\tfrac12\lVert\tilde y\rVert^{2}; by Step 0(a) with a=xa=x and b=y~b=\tilde y, 12∥x−y~∥2=12∥x∥2−x⋅y~+12∥y~∥2\tfrac12\lVert x-\tilde y\rVert^{2}=\tfrac12\lVert x\rVert^{2}-x\cdot\tilde y+\tfrac12\lVert\tilde y\rVert^{2}. Adding, and using claims 1 and 5 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n to write x′⋅y~−x⋅y~=y~⋅(x′−x)x'\cdot\tilde y-x\cdot\tilde y=\tilde y\cdot(x'-x),

ψ(x′)≥12∥x∥2−φ(x)+y~⋅(x′−x)=ψ(x)+y~⋅(x′−x).\psi(x')\ge\tfrac12\lVert x\rVert^{2}-\varphi(x)+\tilde y\cdot(x'-x)=\psi(x)+\tilde y\cdot(x'-x).

Since this holds for every x′∈Rdx'\in\mathbb{R}^{d}, and Rd\mathbb{R}^{d} is convex, y~\tilde y belongs to the subdifferential ∂Rdψ(x)\partial_{\mathbb{R}^{d}}\psi(x).

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