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Proof of Sup- and Inf-Convolutions of Bounded Viscosity Sub- and Supersolutions of the Penalty-Drift Equation with a Convex Penalty

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· 31,477 chars · 42 deps · depth 22 Reason: Proof of the sup/inf-convolution lemma for the penalty-drift equation with a convex penalty.

All structural properties are proved once for the sup-convolution of an arbitrary bounded upper semicontinuous function (attainment by compactness of penalty sublevel sets, semiconvexity as a supremum of affine functions, gradient identification at the maximiser); the inf-convolution case follows by negation. The viscosity inequalities come from transferring a perturbed second-order Taylor majorant of the test function to the maximiser, then using monotonicity of DP, the dissipation inequality, a weighted Young inequality and the modulus of g, and finally letting the perturbation vanish.

Proof

Each result cited below is universally quantified over the data in its own statement, and is applied to the data named at the point of use.

Elementary order and arithmetic manipulations of real numbers (rearranging finite sums, adding inequalities, multiplying an inequality by a nonnegative or by a positive number, reversing an inequality by negation, and the rules for the absolute value) are justified by Elementary Order Arithmetic in an Ordered Field, Elementary Arithmetic in an Ordered Field and Properties of the Absolute Value in an Ordered Field and are not cited individually; the same applies to the vector-space identities in Rn\mathbb{R}^{n}, such as (x+h)−y=(x−y)+h(x+h)-y=(x-y)+h. By clause 2 of the setting the Euclidean distance is dE(x,y)=∥x−y∥d_{E}(x,y)=\lVert x-y\rVert, so local extrema relative to DD and semicontinuity on DD are expressed below through ∥x−y∥\lVert x-y\rVert. We keep the notation p0p_{0}, rr, θ1\theta_{1}, θ2\theta_{2}, g1g_{1}, g2g_{2}, FF, F1F_{1}, F2F_{2} of the statement; in particular p0≤P(y)p_{0}\le P(y) for every y∈Dy\in D.

Step 0 (Preliminaries).

(0.1) Continuity. As recorded in the statement, PP is continuous at every point of DD and hence, by claim 2 of Semicontinuity Under Negation and Characterization of Continuity, both upper and lower semicontinuous on DD. For a fixed a∈Rna\in\mathbb{R}^{n}, the function D→RD\to\mathbb{R} with value 12τ∥y−a∥2=12τdE(y,a)2\tfrac{1}{2\tau}\lVert y-a\rVert^{2}=\tfrac{1}{2\tau}d_{E}(y,a)^{2} at yy is of class C2C^{2} on DD by claim 2 of A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian (with U=DU=D and c=12τc=\tfrac{1}{2\tau}), so the function ea:D→Re_{a}:D\to\mathbb{R}, ea(y)=ηP(y)+12τ∥y−a∥2e_{a}(y)=\eta P(y)+\tfrac{1}{2\tau}\lVert y-a\rVert^{2}, is of class C2C^{2} on DD by claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set; as for PP, it is then continuous at every point of DD (claim 2 of Coordinate Functions, the CkC^k Hierarchy, and Partial Derivatives of a Smooth Map and clause 2 of the calculus setting) and so lower semicontinuous on DD by claim 2 of Semicontinuity Under Negation and Characterization of Continuity.

(0.2) Squares. Let s,s′∈Rs,s'\in\mathbb{R} with 0≤s0\le s and 0≤s′0\le s'. Then s≤s′s\le s' if and only if s2≤s′2s^{2}\le s'^{2}. Indeed, if s≤s′s\le s' then s2≤ss′≤s′2s^{2}\le ss'\le s'^{2}; if instead s′<ss'<s, then 0<s0<s, and s′2≤s′s<sss'^{2}\le s's<ss (the strict step by claim 10 of Elementary Order Arithmetic in an Ordered Field), so s2≤s′2s^{2}\le s'^{2} fails.

(0.3) Expansions. For a,b∈Rna,b\in\mathbb{R}^{n} one has ∥a∥2=a⋅a\lVert a\rVert^{2}=a\cdot a and 0≤∥a∥0\le\lVert a\rVert by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, hence, by Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n (symmetry, additivity and homogeneity in both arguments),

∥a+b∥2=∥a∥2+2 (a⋅b)+∥b∥2,∥a−b∥2=∥a∥2−2 (a⋅b)+∥b∥2.\lVert a+b\rVert^{2}=\lVert a\rVert^{2}+2\,(a\cdot b)+\lVert b\rVert^{2},\qquad \lVert a-b\rVert^{2}=\lVert a\rVert^{2}-2\,(a\cdot b)+\lVert b\rVert^{2}.

Moreover ∥μa∥=∣μ∣ ∥a∥\lVert\mu a\rVert=|\mu|\,\lVert a\rVert for μ∈R\mu\in\mathbb{R} by claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n; in particular ∥a−b∥=∥b−a∥\lVert a-b\rVert=\lVert b-a\rVert, and ∥a−a∥=0\lVert a-a\rVert=0 by claim 3 there.

(0.4) A limiting fact. If a,c∈Ra,c\in\mathbb{R} with 0≤c0\le c satisfy a≤cσa\le c\sigma for every positive σ∈R\sigma\in\mathbb{R}, then a≤0a\le0. Indeed, suppose 0<a0<a. If c=0c=0 then a≤0a\le0, a contradiction; if 0<c0<c, then σ=a2c\sigma=\tfrac{a}{2c} is positive and gives a≤a2<aa\le\tfrac{a}{2}<a, again a contradiction.

Step 1 (A general construction). In Steps 1 to 7, ω:D→R\omega:D\to\mathbb{R} denotes a function that is upper semicontinuous on DD and satisfies ∣ω(y)∣≤M|\omega(y)|\le M, that is −M≤ω(y)≤M-M\le\omega(y)\le M, for every y∈Dy\in D. Put W(y)=ω(y)−ηP(y)W(y)=\omega(y)-\eta P(y) for y∈Dy\in D, and for x,y∈Dx,y\in D put

fx(y)=W(y)−12τ∥x−y∥2.f_{x}(y)=W(y)-\tfrac{1}{2\tau}\lVert x-y\rVert^{2}.

Since p0≤P(y)p_{0}\le P(y) and ω(y)≤M\omega(y)\le M,

−M−ηP(y)≤W(y)≤M−ηp0(y∈D),(1.1)-M-\eta P(y)\le W(y)\le M-\eta p_{0}\qquad(y\in D),\tag{1.1}

and fx(y)≤W(y)f_{x}(y)\le W(y) because 0≤12τ∥x−y∥20\le\tfrac{1}{2\tau}\lVert x-y\rVert^{2}. Hence, exactly as in the statement, for each x∈Dx\in D the set {fx(y):y∈D}\{f_{x}(y):y\in D\} is nonempty and bounded above by M−ηp0M-\eta p_{0}, and we let wω(x)w_{\omega}(x) be its least upper bound, which exists because the real numbers are Dedekind complete. We call y∈Dy\in D an ω\omega-maximiser at xx if wω(x)=fx(y)w_{\omega}(x)=f_{x}(y). For ω=u\omega=u these are the function w‾\overline{w} and the maximisers of Part A. By the definition of a least upper bound, and by (0.3),

fx(y)≤wω(x)for all x,y∈D,fx(x)=W(x)for all x∈D.(1.2)f_{x}(y)\le w_{\omega}(x)\quad\text{for all }x,y\in D,\qquad f_{x}(x)=W(x)\quad\text{for all }x\in D.\tag{1.2}

Step 2 (Existence and location of ω\omega-maximisers). Fix x∈Dx\in D and put t=P(x)+2Mηt=P(x)+\tfrac{2M}{\eta} and L={y∈D:P(y)≤t}L=\{y\in D:P(y)\le t\}, which is compact by the sublevel property of the penalty PP. Let K={y∈D:fx(x)≤fx(y)}K=\{y\in D:f_{x}(x)\le f_{x}(y)\}. If y∈Ky\in K, then by (1.2) W(x)=fx(x)≤fx(y)≤W(y)W(x)=f_{x}(x)\le f_{x}(y)\le W(y), that is ω(x)−ηP(x)≤ω(y)−ηP(y)\omega(x)-\eta P(x)\le\omega(y)-\eta P(y), so ηP(y)≤ω(y)−ω(x)+ηP(x)≤2M+ηP(x)\eta P(y)\le\omega(y)-\omega(x)+\eta P(x)\le2M+\eta P(x) and, dividing by η>0\eta>0, P(y)≤tP(y)\le t. Hence K⊆LK\subseteq L and K={y∈L:fx(x)≤fx(y)}K=\{y\in L:f_{x}(x)\le f_{x}(y)\}.

The function fxf_{x} equals ω−ex\omega-e_{x} on DD with exe_{x} from (0.1) (note ∥x−y∥=∥y−x∥\lVert x-y\rVert=\lVert y-x\rVert). Since ω\omega is upper semicontinuous and exe_{x} is lower semicontinuous on DD, claim 3 of Negation, Restriction, and Separated Differences of Semicontinuous Functions shows that fxf_{x} is upper semicontinuous on DD, and by claim 2 there its restrictions to LL and to KK are upper semicontinuous on LL and on KK. By claim 2 of Compactness of Intersections with Closed Sets and of Level Sets of Semicontinuous Functions (with the compact set LL and c=fx(x)c=f_{x}(x)), KK is compact. It is nonempty, as x∈Kx\in K. By claim 1 of Semicontinuous Functions Attain Their Extrema on a Compact Set there is z∈Kz\in K with fx(y)≤fx(z)f_{x}(y)\le f_{x}(z) for every y∈Ky\in K; and every y∈D∖Ky\in D\setminus K satisfies fx(y)<fx(x)≤fx(z)f_{x}(y)<f_{x}(x)\le f_{x}(z). Thus fx(z)f_{x}(z) is an upper bound of {fx(y):y∈D}\{f_{x}(y):y\in D\} belonging to that set, hence its least upper bound: wω(x)=fx(z)w_{\omega}(x)=f_{x}(z), and zz is an ω\omega-maximiser at xx.

Now let zz be any ω\omega-maximiser at xx. By (1.2), W(x)=fx(x)≤wω(x)=fx(z)=W(z)−12τ∥x−z∥2W(x)=f_{x}(x)\le w_{\omega}(x)=f_{x}(z)=W(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}, so by (1.1)

12τ∥x−z∥2≤W(z)−W(x)≤(M−ηp0)−(−M−ηP(x))=2M+η (P(x)−p0).\tfrac{1}{2\tau}\lVert x-z\rVert^{2}\le W(z)-W(x)\le(M-\eta p_{0})-(-M-\eta P(x))=2M+\eta\,(P(x)-p_{0}).

Multiplying by 2τ>02\tau>0 gives ∥x−z∥2≤r(x)2\lVert x-z\rVert^{2}\le r(x)^{2}, and (0.2) gives

∥x−z∥≤r(x)for every ω-maximiser z at x.(2.1)\lVert x-z\rVert\le r(x)\qquad\text{for every }\omega\text{-maximiser }z\text{ at }x.\tag{2.1}

Step 3 (Bounds). For x∈Dx\in D let zz be an ω\omega-maximiser at xx (Step 2). By (1.2) and (1.1), W(x)=fx(x)≤wω(x)=fx(z)≤W(z)≤M−ηp0W(x)=f_{x}(x)\le w_{\omega}(x)=f_{x}(z)\le W(z)\le M-\eta p_{0}, that is

ω(x)−ηP(x)≤wω(x)≤M−ηp0.(3.1)\omega(x)-\eta P(x)\le w_{\omega}(x)\le M-\eta p_{0}.\tag{3.1}

Step 4 (Semiconvexity and continuity). Let G:D→RG:D\to\mathbb{R}, G(x)=wω(x)+12τ∥x∥2G(x)=w_{\omega}(x)+\tfrac{1}{2\tau}\lVert x\rVert^{2}; since τ−12=12τ\tfrac{\tau^{-1}}{2}=\tfrac{1}{2\tau}, it suffices by Semiconvex Function on a Convex Subset of Rn\mathbb{R}^n to show that GG is convex on DD. For y∈Dy\in D let Ay:Rn→RA_{y}:\mathbb{R}^{n}\to\mathbb{R}, Ay(x)=W(y)−12τ∥y∥2+τ−1(x⋅y)A_{y}(x)=W(y)-\tfrac{1}{2\tau}\lVert y\rVert^{2}+\tau^{-1}(x\cdot y). By (0.3), ∥x−y∥2=∥x∥2−2(x⋅y)+∥y∥2\lVert x-y\rVert^{2}=\lVert x\rVert^{2}-2(x\cdot y)+\lVert y\rVert^{2}, whence

fx(y)+12τ∥x∥2=Ay(x)(x,y∈D).(4.1)f_{x}(y)+\tfrac{1}{2\tau}\lVert x\rVert^{2}=A_{y}(x)\qquad(x,y\in D).\tag{4.1}

By claims 1, 2 and 4 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n, Ay(tx1+(1−t)x2)=t Ay(x1)+(1−t) Ay(x2)A_{y}(t x_{1}+(1-t)x_{2})=t\,A_{y}(x_{1})+(1-t)\,A_{y}(x_{2}) for all x1,x2∈Rnx_{1},x_{2}\in\mathbb{R}^{n} and t∈Rt\in\mathbb{R}. Now let x1,x2∈Dx_{1},x_{2}\in D and t∈Rt\in\mathbb{R} with 0≤t≤10\le t\le1; the point xt=tx1+(1−t)x2x_{t}=t x_{1}+(1-t)x_{2} lies in DD because DD is convex. Choose an ω\omega-maximiser ztz_{t} at xtx_{t} (Step 2). By (4.1) and (1.2), G(xt)=fxt(zt)+12τ∥xt∥2=Azt(xt)G(x_{t})=f_{x_{t}}(z_{t})+\tfrac{1}{2\tau}\lVert x_{t}\rVert^{2}=A_{z_{t}}(x_{t}) and Azt(xi)=fxi(zt)+12τ∥xi∥2≤G(xi)A_{z_{t}}(x_{i})=f_{x_{i}}(z_{t})+\tfrac{1}{2\tau}\lVert x_{i}\rVert^{2}\le G(x_{i}) for i=1,2i=1,2. As 0≤t0\le t and 0≤1−t0\le1-t,

G(xt)=t Azt(x1)+(1−t) Azt(x2)≤t G(x1)+(1−t) G(x2).G(x_{t})=t\,A_{z_{t}}(x_{1})+(1-t)\,A_{z_{t}}(x_{2})\le t\,G(x_{1})+(1-t)\,G(x_{2}).

Hence wωw_{\omega} is semiconvex on DD with constant τ−1\tau^{-1}. Since DD is convex and open, the continuity clause for semiconvex functions (with U=S=DU=S=D) shows: for every x∈Dx\in D and every positive e∈Re\in\mathbb{R} there is a positive δ∈R\delta\in\mathbb{R} such that every y∈Dy\in D with ∥y−x∥<δ\lVert y-x\rVert<\delta satisfies ∣wω(y)−wω(x)∣<e|w_{\omega}(y)-w_{\omega}(x)|<e. We refer to this continuity property as (4.2).

Step 5 (Gradient). Let x∈Dx\in D be such that the partial derivative of wωw_{\omega} with respect to every variable exists at xx, and let zz be an ω\omega-maximiser at xx. Let ψ:D→R\psi:D\to\mathbb{R}, ψ(x′)=−12τ∥x′−z∥2=c dE(x′,z)2\psi(x')=-\tfrac{1}{2\tau}\lVert x'-z\rVert^{2}=c\,d_{E}(x',z)^{2} with c=−12τc=-\tfrac{1}{2\tau}. By claim 1 of A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian (with U=DU=D, a=za=z), for each ii the partial derivative of ψ\psi with respect to the iith variable exists at xx and equals 2c(xi−zi)=τ−1(zi−xi)2c(x_{i}-z_{i})=\tau^{-1}(z_{i}-x_{i}). Let χ=wω−ψ\chi=w_{\omega}-\psi on DD; by claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set (applied to the multiple (−1)ψ(-1)\psi and then to the sum), ∂iχ(x)\partial_{i}\chi(x) exists and ∂iχ(x)=∂iwω(x)−τ−1(zi−xi)\partial_{i}\chi(x)=\partial_{i}w_{\omega}(x)-\tau^{-1}(z_{i}-x_{i}). For every x′∈Dx'\in D, (1.2) gives W(z)+ψ(x′)=fx′(z)≤wω(x′)W(z)+\psi(x')=f_{x'}(z)\le w_{\omega}(x'), that is χ(x′)≥W(z)\chi(x')\ge W(z), while χ(x)=wω(x)−ψ(x)=fx(z)−ψ(x)=W(z)\chi(x)=w_{\omega}(x)-\psi(x)=f_{x}(z)-\psi(x)=W(z) because zz is an ω\omega-maximiser at xx. Hence χ(x′)−χ(x)≥0\chi(x')-\chi(x)\ge0 for every x′∈Dx'\in D.

We claim ℓ:=∂iχ(x)=0\ell:=\partial_{i}\chi(x)=0. For real ss write x(s)=(x1,…,xi−1,xi+s,xi+1,…,xn)x^{(s)}=(x_{1},\dots,x_{i-1},x_{i}+s,x_{i+1},\dots,x_{n}). Suppose 0<ℓ0<\ell. By Partial Derivative on a Euclidean Open Set, applied with the tolerance ℓ\ell, there is a positive δ\delta such that every real ss with 0<∣s∣<δ0<|s|<\delta satisfies x(s)∈Dx^{(s)}\in D and ∣χ(x(s))−χ(x)s−ℓ∣<ℓ\bigl|\tfrac{\chi(x^{(s)})-\chi(x)}{s}-\ell\bigr|<\ell; taking s=−δ2s=-\tfrac{\delta}{2} gives 0<χ(x(s))−χ(x)s0<\tfrac{\chi(x^{(s)})-\chi(x)}{s}, whereas the numerator is nonnegative and s<0s<0, so this quotient is at most 00: a contradiction. Suppose ℓ<0\ell<0. With the tolerance −ℓ-\ell we obtain δ\delta as before, and s=δ2s=\tfrac{\delta}{2} gives χ(x(s))−χ(x)s<0\tfrac{\chi(x^{(s)})-\chi(x)}{s}<0, whereas the quotient is nonnegative: a contradiction. As the order is total, ℓ=0\ell=0. Therefore ∂iwω(x)=τ−1(zi−xi)\partial_{i}w_{\omega}(x)=\tau^{-1}(z_{i}-x_{i}) for every ii, and by Gradient of a Real-Valued Function on a Euclidean Open Set together with the coordinatewise definitions of the difference and the scalar multiple,

Dwω(x)=τ−1(z−x),∥Dwω(x)∥=τ−1∥x−z∥≤τ−1r(x),(5.1)Dw_{\omega}(x)=\tau^{-1}(z-x),\qquad \lVert Dw_{\omega}(x)\rVert=\tau^{-1}\lVert x-z\rVert\le\tau^{-1}r(x),\tag{5.1}

the equality by (0.3) and the inequality by (2.1).

Step 6 (Transfer between points). Let x,y∈Dx,y\in D and let zz be an ω\omega-maximiser at xx. By (1.2), W(z)−12τ∥y−z∥2=fy(z)≤wω(y)W(z)-\tfrac{1}{2\tau}\lVert y-z\rVert^{2}=f_{y}(z)\le w_{\omega}(y), and wω(x)=W(z)−12τ∥x−z∥2w_{\omega}(x)=W(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}, so

wω(x)−wω(y)≤12τ(∥y−z∥2−∥x−z∥2).w_{\omega}(x)-w_{\omega}(y)\le\tfrac{1}{2\tau}\bigl(\lVert y-z\rVert^{2}-\lVert x-z\rVert^{2}\bigr).

By claim 6 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and (0.3), ∥y−z∥=∥(y−x)+(x−z)∥≤∥x−y∥+∥x−z∥\lVert y-z\rVert=\lVert(y-x)+(x-z)\rVert\le\lVert x-y\rVert+\lVert x-z\rVert, so by (0.2) ∥y−z∥2≤∥x−y∥2+2∥x−y∥∥x−z∥+∥x−z∥2\lVert y-z\rVert^{2}\le\lVert x-y\rVert^{2}+2\lVert x-y\rVert\lVert x-z\rVert+\lVert x-z\rVert^{2} and

wω(x)−wω(y)≤12τ(∥x−y∥2+2∥x−y∥∥x−z∥).(6.1)w_{\omega}(x)-w_{\omega}(y)\le\tfrac{1}{2\tau}\bigl(\lVert x-y\rVert^{2}+2\lVert x-y\rVert\lVert x-z\rVert\bigr).\tag{6.1}

Next, by (1.2), W(y)−12τ∥x−y∥2=fx(y)≤wω(x)=W(z)−12τ∥x−z∥2W(y)-\tfrac{1}{2\tau}\lVert x-y\rVert^{2}=f_{x}(y)\le w_{\omega}(x)=W(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}, so by (1.1)

∥x−z∥2≤2τ(W(z)−W(y))+∥x−y∥2≤2τ(2M+η(P(y)−p0))+∥x−y∥2=r(y)2+∥x−y∥2,\lVert x-z\rVert^{2}\le2\tau\bigl(W(z)-W(y)\bigr)+\lVert x-y\rVert^{2}\le2\tau\bigl(2M+\eta(P(y)-p_{0})\bigr)+\lVert x-y\rVert^{2}=r(y)^{2}+\lVert x-y\rVert^{2},

which is at most (r(y)+∥x−y∥)2\bigl(r(y)+\lVert x-y\rVert\bigr)^{2} because 0≤2r(y)∥x−y∥0\le2r(y)\lVert x-y\rVert. By (0.2), ∥x−z∥≤r(y)+∥x−y∥\lVert x-z\rVert\le r(y)+\lVert x-y\rVert. Inserting this into (6.1), using 0≤2∥x−y∥0\le2\lVert x-y\rVert,

wω(x)−wω(y)≤12τ(3∥x−y∥2+2∥x−y∥ r(y))=12τ∥x−y∥(3∥x−y∥+2r(y)).(6.2)w_{\omega}(x)-w_{\omega}(y)\le\tfrac{1}{2\tau}\bigl(3\lVert x-y\rVert^{2}+2\lVert x-y\rVert\,r(y)\bigr)=\tfrac{1}{2\tau}\lVert x-y\rVert\bigl(3\lVert x-y\rVert+2r(y)\bigr).\tag{6.2}

Step 7 (Transfer of test functions).

(7a) Let φ:D→R\varphi:D\to\mathbb{R} be of class C2C^{2} on DD, let x∈Dx\in D, suppose that wω−φw_{\omega}-\varphi has a local maximum at xx relative to DD, let zz be an ω\omega-maximiser at xx, and put p=Dφ(x)p=D\varphi(x) and X=D2φ(x)∈S(n)X=D^{2}\varphi(x)\in\mathcal{S}(n). Then p=τ−1(z−x)p=\tau^{-1}(z-x).

Indeed, let β1\beta_{1} be positive such that every x′∈Dx'\in D with ∥x−x′∥<β1\lVert x-x'\rVert<\beta_{1} satisfies wω(x′)−φ(x′)≤wω(x)−φ(x)w_{\omega}(x')-\varphi(x')\le w_{\omega}(x)-\varphi(x). Let ψ\psi be as in Step 5 (with this zz); it is of class C2C^{2} on DD with Dψ(x)=(2c)(x−z)=τ−1(z−x)D\psi(x)=(2c)(x-z)=\tau^{-1}(z-x), by claims 2 and 3 of A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian. For x′∈Dx'\in D with ∥x−x′∥<β1\lVert x-x'\rVert<\beta_{1}, (1.2) gives

W(z)+ψ(x′)=fx′(z)≤wω(x′)≤wω(x)+φ(x′)−φ(x)=W(z)+ψ(x)+φ(x′)−φ(x),W(z)+\psi(x')=f_{x'}(z)\le w_{\omega}(x')\le w_{\omega}(x)+\varphi(x')-\varphi(x)=W(z)+\psi(x)+\varphi(x')-\varphi(x),

that is φ(x)−ψ(x)≤φ(x′)−ψ(x′)\varphi(x)-\psi(x)\le\varphi(x')-\psi(x'). So φ−ψ\varphi-\psi, which is of class C2C^{2} on DD by claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, has a local minimum at xx relative to DD, and its gradient at xx is the origin by claim 2 of First- and Second-Order Conditions at a Local Extremum of a Function of Class C2C^2. By claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set that gradient is Dφ(x)−Dψ(x)D\varphi(x)-D\psi(x), so p=Dψ(x)=τ−1(z−x)p=D\psi(x)=\tau^{-1}(z-x).

(7b) In the situation of (7a), for every positive σ∈R\sigma\in\mathbb{R} there is a positive β∈R\beta\in\mathbb{R} such that every y∈Dy\in D with ∥y−z∥<β\lVert y-z\rVert<\beta satisfies

W(y)≤W(z)+p⋅(y−z)+12 (y−z)⋅((X+σIn)(y−z)).(7.1)W(y)\le W(z)+p\cdot(y-z)+\tfrac{1}{2}\,(y-z)\cdot\bigl((X+\sigma I_{n})(y-z)\bigr).\tag{7.1}

Indeed, X+σIn∈S(n)X+\sigma I_{n}\in\mathcal{S}(n) by the clause on symmetric matrices. By Second-Order Taylor Expansion with Peano Remainder (with U=DU=D, f=φf=\varphi and the tolerance σ2\tfrac{\sigma}{2}) there is a positive β2\beta_{2} such that every h∈Rnh\in\mathbb{R}^{n} with ∥h∥<β2\lVert h\rVert<\beta_{2} satisfies x+h∈Dx+h\in D and

∣φ(x+h)−φ(x)−∑i=1n∂iφ(x) hi−12∑i=1n∑j=1n∂j∂iφ(x) hihj∣≤σ2∥h∥2,\Bigl|\varphi(x+h)-\varphi(x)-\sum_{i=1}^{n}\partial_{i}\varphi(x)\,h_{i}-\tfrac{1}{2}\sum_{i=1}^{n}\sum_{j=1}^{n}\partial_{j}\partial_{i}\varphi(x)\,h_{i}h_{j}\Bigr|\le\tfrac{\sigma}{2}\lVert h\rVert^{2},

the distance from hh to the origin used there being ∥h∥\lVert h\rVert by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. By Gradient of a Real-Valued Function on a Euclidean Open Set and the definition of the dot product, ∑i∂iφ(x)hi=p⋅h\sum_{i}\partial_{i}\varphi(x)h_{i}=p\cdot h. By Hessian Matrix of a C^2 Function, ∂j∂iφ(x)\partial_{j}\partial_{i}\varphi(x) is the entry XjiX_{ji}, which equals XijX_{ij} as XX is symmetric, so claim 4 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum gives ∑i∑j∂j∂iφ(x)hihj=h⋅(Xh)\sum_{i}\sum_{j}\partial_{j}\partial_{i}\varphi(x)h_{i}h_{j}=h\cdot(Xh). By claims 1 and 2 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum, (X+σIn)h=Xh+σh(X+\sigma I_{n})h=Xh+\sigma h, so h⋅((X+σIn)h)=h⋅(Xh)+σ∥h∥2h\cdot((X+\sigma I_{n})h)=h\cdot(Xh)+\sigma\lVert h\rVert^{2} by Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n and (0.3). Consequently

φ(x+h)−φ(x)≤p⋅h+12 h⋅((X+σIn)h)whenever ∥h∥<β2.(7.2)\varphi(x+h)-\varphi(x)\le p\cdot h+\tfrac{1}{2}\,h\cdot\bigl((X+\sigma I_{n})h\bigr)\qquad\text{whenever }\lVert h\rVert<\beta_{2}.\tag{7.2}

Let β1\beta_{1} be as in (7a) and let β\beta be the lesser of β1\beta_{1} and β2\beta_{2} (claim 9 of Elementary Order Arithmetic in an Ordered Field). Let y∈Dy\in D with ∥y−z∥<β\lVert y-z\rVert<\beta, and put h=y−zh=y-z and x′=x+hx'=x+h. Then ∥h∥<β2\lVert h\rVert<\beta_{2}, so x′∈Dx'\in D and (7.2) holds; and ∥x−x′∥=∥h∥<β1\lVert x-x'\rVert=\lVert h\rVert<\beta_{1}, so wω(x′)≤wω(x)+φ(x′)−φ(x)w_{\omega}(x')\le w_{\omega}(x)+\varphi(x')-\varphi(x). Since x′−y=x−zx'-y=x-z, (1.2) gives W(y)−12τ∥x−z∥2=fx′(y)≤wω(x′)W(y)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}=f_{x'}(y)\le w_{\omega}(x'). Together with wω(x)=fx(z)=W(z)−12τ∥x−z∥2w_{\omega}(x)=f_{x}(z)=W(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2} and (7.2) this yields

W(y)−12τ∥x−z∥2≤W(z)−12τ∥x−z∥2+p⋅h+12 h⋅((X+σIn)h),W(y)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}\le W(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}+p\cdot h+\tfrac{1}{2}\,h\cdot\bigl((X+\sigma I_{n})h\bigr),

which is (7.1).

(7c) Let z∈Dz\in D, p∈Rnp\in\mathbb{R}^{n}, B∈S(n)B\in\mathcal{S}(n) and μ∈R\mu\in\mathbb{R}, and let Ψ:D→R\Psi:D\to\mathbb{R}, Ψ(y)=12(y−z)⋅(B(y−z))+p⋅(y−z)+μP(y)\Psi(y)=\tfrac{1}{2}(y-z)\cdot(B(y-z))+p\cdot(y-z)+\mu P(y). Then Ψ\Psi is of class C2C^{2} on DD, and

Ψ(z)=μP(z),DΨ(z)=p+μ DP(z),D2Ψ(z)=B+μ D2P(z).\Psi(z)=\mu P(z),\qquad D\Psi(z)=p+\mu\,DP(z),\qquad D^{2}\Psi(z)=B+\mu\,D^{2}P(z).

Indeed, by the clause on quadratic functions the function Q^:Rn→R\hat{Q}:\mathbb{R}^{n}\to\mathbb{R}, Q^(h)=12h⋅(Bh)+p⋅h+0\hat{Q}(h)=\tfrac{1}{2}h\cdot(Bh)+p\cdot h+0, is of class C2C^{2} on Rn\mathbb{R}^{n} with DQ^(h)=Bh+pD\hat{Q}(h)=Bh+p and D2Q^(h)=BD^{2}\hat{Q}(h)=B; by the translation clause (with V=RnV=\mathbb{R}^{n} and b=−zb=-z, so that V−b=RnV-b=\mathbb{R}^{n}), Q(y)=Q^(y−z)Q(y)=\hat{Q}(y-z) is of class C2C^{2} on Rn\mathbb{R}^{n} with DQ(y)=B(y−z)+pDQ(y)=B(y-z)+p and D2Q(y)=BD^{2}Q(y)=B; and by clause 2 of the calculus setting its restriction to DD is of class C2C^{2} on DD with the same gradient and Hessian. As PP is of class C2C^{2} on DD, claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set shows that Ψ\Psi is of class C2C^{2} on DD. Claim 1 there, applied first to the partial derivatives of QQ and μP\mu P at every point of DD and then to the partial derivatives of the functions ∂jQ\partial_{j}Q and μ ∂jP\mu\,\partial_{j}P (which exist because QQ and PP are of class C2C^{2}), gives ∂iΨ(z)=∂iQ(z)+μ ∂iP(z)\partial_{i}\Psi(z)=\partial_{i}Q(z)+\mu\,\partial_{i}P(z) and ∂i∂jΨ(z)=∂i∂jQ(z)+μ ∂i∂jP(z)\partial_{i}\partial_{j}\Psi(z)=\partial_{i}\partial_{j}Q(z)+\mu\,\partial_{i}\partial_{j}P(z) for all i,ji,j. By Gradient of a Real-Valued Function on a Euclidean Open Set, Hessian Matrix of a C^2 Function and the entrywise definitions of sums and scalar multiples, DΨ(z)=B(z−z)+p+μDP(z)=p+μDP(z)D\Psi(z)=B(z-z)+p+\mu DP(z)=p+\mu DP(z) (as BB applied to the origin is the origin, by claim 3 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum with the scalar 00) and D2Ψ(z)=B+μD2P(z)D^{2}\Psi(z)=B+\mu D^{2}P(z); finally Ψ(z)=μP(z)\Psi(z)=\mu P(z) because every dot product with the origin vanishes.

Step 8 (Part A, clauses A1 to A5). By Viscosity Subsolution and Supersolution of a Second-Order Equation, uu is upper semicontinuous on DD, and ∣u(y)∣≤M|u(y)|\le M for y∈Dy\in D; so Steps 1 to 7 apply with ω=u\omega=u, for which wu=w‾w_{u}=\overline{w} and the uu-maximisers at xx are the maximisers at xx of Part A. Clause A1 is Step 2 with (2.1); clause A2 is (3.1); clause A3 is Step 4; clause A4 is (5.1), the parenthetical remark in A4 being claim 1 of A Derivative Matrix is the Jacobian Matrix, and is Unique applied to the single coordinate function w‾\overline{w}; clause A5 is (6.2).

Step 9 (Part A, clause A6). Semicontinuity. Let x∈Dx\in D and let ee be positive; by (4.2) with ω=u\omega=u there is a positive δ\delta such that every y∈Dy\in D with ∥x−y∥<δ\lVert x-y\rVert<\delta satisfies ∣w‾(y)−w‾(x)∣<e|\overline{w}(y)-\overline{w}(x)|<e, hence w‾(y)<w‾(x)+e\overline{w}(y)<\overline{w}(x)+e. So w‾\overline{w} is upper semicontinuous on DD.

The subsolution inequality. Let φ:D→R\varphi:D\to\mathbb{R} be of class C2C^{2} on DD and let x∈Dx\in D be such that w‾−φ\overline{w}-\varphi has a local maximum at xx relative to DD. Choose, in this order: a maximiser zz at xx (clause A1); put p=Dφ(x)p=D\varphi(x), X=D2φ(x)X=D^{2}\varphi(x), ξ=DP(z)\xi=DP(z) and H=D2P(z)H=D^{2}P(z); fix a positive σ∈R\sigma\in\mathbb{R}; and let β\beta be given by (7b) for this σ\sigma (with ω=u\omega=u, so W=u−ηPW=u-\eta P). By (7a), p=τ−1(z−x)p=\tau^{-1}(z-x). Let Ψ\Psi be the function of (7c) with B=X+σInB=X+\sigma I_{n} and μ=η\mu=\eta. For y∈Dy\in D with ∥y−z∥<β\lVert y-z\rVert<\beta, (7.1) reads u(y)−Ψ(y)≤u(z)−ηP(z)=u(z)−Ψ(z)u(y)-\Psi(y)\le u(z)-\eta P(z)=u(z)-\Psi(z); thus u−Ψu-\Psi has a local maximum at zz relative to DD. Since uu is a viscosity subsolution of FF on DD and Ψ\Psi is of class C2C^{2} on DD with DΨ(z)=p+ηξD\Psi(z)=p+\eta\xi and D2Ψ(z)=X+σIn+ηHD^{2}\Psi(z)=X+\sigma I_{n}+\eta H, Viscosity Subsolution and Supersolution of a Second-Order Equation and the formula for FF give

λu(z)+θ2∥p+ηξ∥2+ξ⋅(p+ηξ)−κ2tr⁡(X+σIn+ηH)−g(z)≤0.\lambda u(z)+\tfrac{\theta}{2}\lVert p+\eta\xi\rVert^{2}+\xi\cdot(p+\eta\xi)-\tfrac{\kappa}{2}\operatorname{tr}\bigl(X+\sigma I_{n}+\eta H\bigr)-g(z)\le0 .

By claim 1 of Basic Properties of the Trace, tr⁡(X+σIn+ηH)=tr⁡X+σtr⁡In+ηtr⁡H\operatorname{tr}(X+\sigma I_{n}+\eta H)=\operatorname{tr}X+\sigma\operatorname{tr}I_{n}+\eta\operatorname{tr}H, and tr⁡In=n\operatorname{tr}I_{n}=n (the sum of nn ones) by Trace of a Real Square Matrix and Identity Matrix. By (0.3) and Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n, ∥p+ηξ∥2=∥p∥2+2η(p⋅ξ)+η2∥ξ∥2\lVert p+\eta\xi\rVert^{2}=\lVert p\rVert^{2}+2\eta(p\cdot\xi)+\eta^{2}\lVert\xi\rVert^{2} and ξ⋅(p+ηξ)=ξ⋅p+η∥ξ∥2\xi\cdot(p+\eta\xi)=\xi\cdot p+\eta\lVert\xi\rVert^{2}. Hence

λu(z)+θ2∥p∥2+θη (p⋅ξ)+θη22∥ξ∥2+ξ⋅p+η∥ξ∥2−κ2tr⁡X−κ2nσ−κη2tr⁡H≤g(z).(9.1)\lambda u(z)+\tfrac{\theta}{2}\lVert p\rVert^{2}+\theta\eta\,(p\cdot\xi)+\tfrac{\theta\eta^{2}}{2}\lVert\xi\rVert^{2}+\xi\cdot p+\eta\lVert\xi\rVert^{2}-\tfrac{\kappa}{2}\operatorname{tr}X-\tfrac{\kappa}{2}n\sigma-\tfrac{\kappa\eta}{2}\operatorname{tr}H\le g(z).\tag{9.1}

We bound three of these terms from below. First, the dissipation inequality at zz, multiplied by η>0\eta>0, gives κη2tr⁡H≤η(1−ε)∥ξ∥2+ηλP(z)+ηC\tfrac{\kappa\eta}{2}\operatorname{tr}H\le\eta(1-\varepsilon)\lVert\xi\rVert^{2}+\eta\lambda P(z)+\eta C. Second, 0≤θη22∥ξ∥20\le\tfrac{\theta\eta^{2}}{2}\lVert\xi\rVert^{2}. Third, the weighted Young inequality, applied to the points −θp-\theta p and ξ\xi with the positive number t=(2ε)−1t=(2\varepsilon)^{-1} (its remaining data BB and ε\varepsilon play no role in that clause and may be taken to be InI_{n} and 11), gives 2((−θp)⋅ξ)≤12ε∥−θp∥2+2ε∥ξ∥2=θ22ε∥p∥2+2ε∥ξ∥22\bigl((-\theta p)\cdot\xi\bigr)\le\tfrac{1}{2\varepsilon}\lVert-\theta p\rVert^{2}+2\varepsilon\lVert\xi\rVert^{2}=\tfrac{\theta^{2}}{2\varepsilon}\lVert p\rVert^{2}+2\varepsilon\lVert\xi\rVert^{2} (using ∥−θp∥=θ∥p∥\lVert-\theta p\rVert=\theta\lVert p\rVert from (0.3)); since (−θp)⋅ξ=−θ (p⋅ξ)(-\theta p)\cdot\xi=-\theta\,(p\cdot\xi) by claim 4 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n, halving and multiplying by η\eta gives θη (p⋅ξ)≥−θ2η4ε∥p∥2−ηε∥ξ∥2\theta\eta\,(p\cdot\xi)\ge-\tfrac{\theta^{2}\eta}{4\varepsilon}\lVert p\rVert^{2}-\eta\varepsilon\lVert\xi\rVert^{2}. Inserting the three bounds into (9.1), and using η∥ξ∥2−η(1−ε)∥ξ∥2−ηε∥ξ∥2=0\eta\lVert\xi\rVert^{2}-\eta(1-\varepsilon)\lVert\xi\rVert^{2}-\eta\varepsilon\lVert\xi\rVert^{2}=0 and θ2−θ2η4ε=θ12\tfrac{\theta}{2}-\tfrac{\theta^{2}\eta}{4\varepsilon}=\tfrac{\theta_{1}}{2},

λ(u(z)−ηP(z))+θ12∥p∥2+ξ⋅p−κ2tr⁡X−κ2nσ≤g(z)+ηC.(9.2)\lambda\bigl(u(z)-\eta P(z)\bigr)+\tfrac{\theta_{1}}{2}\lVert p\rVert^{2}+\xi\cdot p-\tfrac{\kappa}{2}\operatorname{tr}X-\tfrac{\kappa}{2}n\sigma\le g(z)+\eta C.\tag{9.2}

Now we compare with the point xx. (i) Since zz is a maximiser at xx, w‾(x)=u(z)−ηP(z)−12τ∥x−z∥2≤u(z)−ηP(z)\overline{w}(x)=u(z)-\eta P(z)-\tfrac{1}{2\tau}\lVert x-z\rVert^{2}\le u(z)-\eta P(z), so λw‾(x)≤λ(u(z)−ηP(z))\lambda\overline{w}(x)\le\lambda(u(z)-\eta P(z)). (ii) The monotonicity hypothesis with the points xx and zz gives 0≤(DP(x)−ξ)⋅(x−z)0\le(DP(x)-\xi)\cdot(x-z); as p=−τ−1(x−z)p=-\tau^{-1}(x-z), Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n gives ξ⋅p−DP(x)⋅p=τ−1((DP(x)−ξ)⋅(x−z))≥0\xi\cdot p-DP(x)\cdot p=\tau^{-1}\bigl((DP(x)-\xi)\cdot(x-z)\bigr)\ge0, so DP(x)⋅p≤ξ⋅pDP(x)\cdot p\le\xi\cdot p. (iii) By the hypothesis on gg, g(z)−g(x)≤∣g(x)−g(z)∣≤ρ(∥x−z∥)≤ρ(r(x))g(z)-g(x)\le|g(x)-g(z)|\le\rho(\lVert x-z\rVert)\le\rho(r(x)), the last step because ∥x−z∥≤r(x)\lVert x-z\rVert\le r(x) by clause A1 and ρ\rho is nondecreasing; so g(z)+ηC≤g1(x)g(z)+\eta C\le g_{1}(x). Combining (i), (ii), (iii) with (9.2),

F1(x,w‾(x),Dφ(x),D2φ(x))=λw‾(x)+θ12∥p∥2+DP(x)⋅p−κ2tr⁡X−g1(x)≤κ2n σ.F_{1}\bigl(x,\overline{w}(x),D\varphi(x),D^{2}\varphi(x)\bigr)=\lambda\overline{w}(x)+\tfrac{\theta_{1}}{2}\lVert p\rVert^{2}+DP(x)\cdot p-\tfrac{\kappa}{2}\operatorname{tr}X-g_{1}(x)\le\tfrac{\kappa}{2}n\,\sigma .

The left-hand side does not depend on σ\sigma, and 0≤κ2n0\le\tfrac{\kappa}{2}n; as σ\sigma was an arbitrary positive number, (0.4) gives F1(x,w‾(x),Dφ(x),D2φ(x))≤0F_{1}(x,\overline{w}(x),D\varphi(x),D^{2}\varphi(x))\le0. Since φ\varphi and xx were arbitrary and w‾\overline{w} is upper semicontinuous, w‾\overline{w} is a viscosity subsolution of F1F_{1} on DD by Viscosity Subsolution and Supersolution of a Second-Order Equation; this is clause A6.

Step 10 (Part B, clauses B1 to B5). By Viscosity Subsolution and Supersolution of a Second-Order Equation, vv is lower semicontinuous on DD, so −v-v is upper semicontinuous on DD by claim 1 of Semicontinuity Under Negation and Characterization of Continuity; and ∣−v(y)∣=∣v(y)∣≤M|-v(y)|=|v(y)|\le M. Hence Steps 1 to 7 apply with ω=−v\omega=-v; then W(y)=−v(y)−ηP(y)W(y)=-v(y)-\eta P(y) and fx(y)=−(v(y)+ηP(y)+12τ∥x−y∥2)f_{x}(y)=-\bigl(v(y)+\eta P(y)+\tfrac{1}{2\tau}\lVert x-y\rVert^{2}\bigr). For x∈Dx\in D, the set of additive inverses of the elements of the set displayed in Part B is therefore {fx(y):y∈D}\{f_{x}(y):y\in D\}, whose least upper bound is w−v(x)w_{-v}(x); by the definition of w‾\underline{w} in the statement,

w‾(x)=−w−v(x)(x∈D),(10.1)\underline{w}(x)=-w_{-v}(x)\qquad(x\in D),\tag{10.1}

and (by reversing inequalities under negation) this number is indeed the greatest lower bound of the set displayed in Part B. Moreover y∈Dy\in D is a minimiser at xx if and only if it is a (−v)(-v)-maximiser at xx. Clause B1 is therefore Step 2 with (2.1). Clause B2 follows from (3.1), which reads −v(x)−ηP(x)≤−w‾(x)≤M−ηp0-v(x)-\eta P(x)\le-\underline{w}(x)\le M-\eta p_{0}, by negation. Clause B3 is Step 4, since −w‾=w−v-\underline{w}=w_{-v}. For clause B4: since w−v=(−1)w‾w_{-v}=(-1)\underline{w} and w‾=(−1)w−v\underline{w}=(-1)w_{-v}, claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set shows that the partial derivatives of w‾\underline{w} at xx exist exactly when those of w−vw_{-v} do, with ∂iw‾(x)=−∂iw−v(x)\partial_{i}\underline{w}(x)=-\partial_{i}w_{-v}(x); so by (5.1) Dw‾(x)=−τ−1(y−x)=τ−1(x−y)D\underline{w}(x)=-\tau^{-1}(y-x)=\tau^{-1}(x-y) for every minimiser yy at xx, and ∥Dw‾(x)∥=∥Dw−v(x)∥≤τ−1r(x)\lVert D\underline{w}(x)\rVert=\lVert Dw_{-v}(x)\rVert\le\tau^{-1}r(x) by (0.3); the parenthetical remark is again claim 1 of A Derivative Matrix is the Jacobian Matrix, and is Unique. Clause B5 follows from (6.2) with ω=−v\omega=-v, which reads −w‾(x)≤−w‾(y)+12τ∥x−y∥(3∥x−y∥+2r(y))-\underline{w}(x)\le-\underline{w}(y)+\tfrac{1}{2\tau}\lVert x-y\rVert(3\lVert x-y\rVert+2r(y)), by negation.

Step 11 (Part B, clause B6). Semicontinuity. Let x∈Dx\in D and let ee be positive; by (4.2) with ω=−v\omega=-v there is a positive δ\delta such that every y∈Dy\in D with ∥x−y∥<δ\lVert x-y\rVert<\delta satisfies ∣w‾(y)−w‾(x)∣=∣w−v(y)−w−v(x)∣<e|\underline{w}(y)-\underline{w}(x)|=|w_{-v}(y)-w_{-v}(x)|<e, hence w‾(x)−e<w‾(y)\underline{w}(x)-e<\underline{w}(y). So w‾\underline{w} is lower semicontinuous on DD.

The supersolution inequality. Let φ:D→R\varphi:D\to\mathbb{R} be of class C2C^{2} on DD and let x∈Dx\in D be such that w‾−φ\underline{w}-\varphi has a local minimum at xx relative to DD. By (10.1), w−v−(−φ)=−(w‾−φ)w_{-v}-(-\varphi)=-(\underline{w}-\varphi) has a local maximum at xx relative to DD (with the same radius), and −φ=(−1)φ-\varphi=(-1)\varphi is of class C2C^{2} on DD with D(−φ)(x)=−Dφ(x)D(-\varphi)(x)=-D\varphi(x) and D2(−φ)(x)=−D2φ(x)D^{2}(-\varphi)(x)=-D^{2}\varphi(x), by claims 1 and 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set. Choose, in this order: a minimiser zz at xx (clause B1), which is a (−v)(-v)-maximiser at xx; put p=Dφ(x)p=D\varphi(x), X=D2φ(x)X=D^{2}\varphi(x), ξ=DP(z)\xi=DP(z) and H=D2P(z)H=D^{2}P(z); fix a positive σ∈R\sigma\in\mathbb{R}; and let β\beta be given by (7b) for ω=−v\omega=-v, the test function −φ-\varphi (whose gradient and Hessian at xx are −p-p and −X-X) and this σ\sigma. By (7a), −p=τ−1(z−x)-p=\tau^{-1}(z-x), that is p=τ−1(x−z)p=\tau^{-1}(x-z). For y∈Dy\in D with ∥y−z∥<β\lVert y-z\rVert<\beta, (7.1) reads

−v(y)−ηP(y)≤−v(z)−ηP(z)+(−p)⋅(y−z)+12(y−z)⋅((−X+σIn)(y−z)).-v(y)-\eta P(y)\le-v(z)-\eta P(z)+(-p)\cdot(y-z)+\tfrac{1}{2}(y-z)\cdot\bigl((-X+\sigma I_{n})(y-z)\bigr).

By claim 1 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum and Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n, (−p)⋅(y−z)=− p⋅(y−z)(-p)\cdot(y-z)=-\,p\cdot(y-z) and (y−z)⋅((−X+σIn)(y−z))=−(y−z)⋅((X−σIn)(y−z))(y-z)\cdot((-X+\sigma I_{n})(y-z))=-(y-z)\cdot((X-\sigma I_{n})(y-z)), where X−σIn∈S(n)X-\sigma I_{n}\in\mathcal{S}(n); negating,

v(y)+ηP(y)≥v(z)+ηP(z)+p⋅(y−z)+12(y−z)⋅((X−σIn)(y−z)).v(y)+\eta P(y)\ge v(z)+\eta P(z)+p\cdot(y-z)+\tfrac{1}{2}(y-z)\cdot\bigl((X-\sigma I_{n})(y-z)\bigr).

Let Ψ\Psi be the function of (7c) with B=X−σInB=X-\sigma I_{n} and μ=−η\mu=-\eta. The last inequality says v(y)−Ψ(y)≥v(z)+ηP(z)=v(z)−Ψ(z)v(y)-\Psi(y)\ge v(z)+\eta P(z)=v(z)-\Psi(z) for y∈Dy\in D with ∥y−z∥<β\lVert y-z\rVert<\beta, so v−Ψv-\Psi has a local minimum at zz relative to DD. Since vv is a viscosity supersolution of FF on DD and DΨ(z)=p−ηξD\Psi(z)=p-\eta\xi, D2Ψ(z)=X−σIn−ηHD^{2}\Psi(z)=X-\sigma I_{n}-\eta H, we obtain, with claim 1 of Basic Properties of the Trace and tr⁡In=n\operatorname{tr}I_{n}=n as in Step 9, and with (0.3),

g(z)≤λv(z)+θ2∥p−ηξ∥2+ξ⋅p−η∥ξ∥2−κ2tr⁡X+κ2nσ+κη2tr⁡H.(11.1)g(z)\le\lambda v(z)+\tfrac{\theta}{2}\lVert p-\eta\xi\rVert^{2}+\xi\cdot p-\eta\lVert\xi\rVert^{2}-\tfrac{\kappa}{2}\operatorname{tr}X+\tfrac{\kappa}{2}n\sigma+\tfrac{\kappa\eta}{2}\operatorname{tr}H .\tag{11.1}

We bound two terms from above. First, as in Step 9, κη2tr⁡H≤η(1−ε)∥ξ∥2+ηλP(z)+ηC\tfrac{\kappa\eta}{2}\operatorname{tr}H\le\eta(1-\varepsilon)\lVert\xi\rVert^{2}+\eta\lambda P(z)+\eta C. Second, by (0.3), θ2∥p−ηξ∥2=θ2∥p∥2−θη (p⋅ξ)+θη22∥ξ∥2\tfrac{\theta}{2}\lVert p-\eta\xi\rVert^{2}=\tfrac{\theta}{2}\lVert p\rVert^{2}-\theta\eta\,(p\cdot\xi)+\tfrac{\theta\eta^{2}}{2}\lVert\xi\rVert^{2}; here θη22∥ξ∥2=η2(θη)∥ξ∥2≤ηε2∥ξ∥2\tfrac{\theta\eta^{2}}{2}\lVert\xi\rVert^{2}=\tfrac{\eta}{2}(\theta\eta)\lVert\xi\rVert^{2}\le\tfrac{\eta\varepsilon}{2}\lVert\xi\rVert^{2} because θη≤ε\theta\eta\le\varepsilon; and the weighted Young inequality, applied to the points −θp-\theta p and ξ\xi with t=ε−1t=\varepsilon^{-1}, gives 2((−θp)⋅ξ)≤θ2ε∥p∥2+ε∥ξ∥22\bigl((-\theta p)\cdot\xi\bigr)\le\tfrac{\theta^{2}}{\varepsilon}\lVert p\rVert^{2}+\varepsilon\lVert\xi\rVert^{2}, whence, as (−θp)⋅ξ=−θ (p⋅ξ)(-\theta p)\cdot\xi=-\theta\,(p\cdot\xi), −θη (p⋅ξ)≤θ2η2ε∥p∥2+ηε2∥ξ∥2-\theta\eta\,(p\cdot\xi)\le\tfrac{\theta^{2}\eta}{2\varepsilon}\lVert p\rVert^{2}+\tfrac{\eta\varepsilon}{2}\lVert\xi\rVert^{2}. Since θ2+θ2η2ε=θ22\tfrac{\theta}{2}+\tfrac{\theta^{2}\eta}{2\varepsilon}=\tfrac{\theta_{2}}{2}, this gives θ2∥p−ηξ∥2≤θ22∥p∥2+ηε∥ξ∥2\tfrac{\theta}{2}\lVert p-\eta\xi\rVert^{2}\le\tfrac{\theta_{2}}{2}\lVert p\rVert^{2}+\eta\varepsilon\lVert\xi\rVert^{2}. Inserting both bounds into (11.1) and using −η∥ξ∥2+η(1−ε)∥ξ∥2+ηε∥ξ∥2=0-\eta\lVert\xi\rVert^{2}+\eta(1-\varepsilon)\lVert\xi\rVert^{2}+\eta\varepsilon\lVert\xi\rVert^{2}=0,

g(z)−ηC≤λ(v(z)+ηP(z))+θ22∥p∥2+ξ⋅p−κ2tr⁡X+κ2nσ.(11.2)g(z)-\eta C\le\lambda\bigl(v(z)+\eta P(z)\bigr)+\tfrac{\theta_{2}}{2}\lVert p\rVert^{2}+\xi\cdot p-\tfrac{\kappa}{2}\operatorname{tr}X+\tfrac{\kappa}{2}n\sigma .\tag{11.2}

Now we compare with the point xx. (i) Since zz is a minimiser at xx, w‾(x)=v(z)+ηP(z)+12τ∥x−z∥2≥v(z)+ηP(z)\underline{w}(x)=v(z)+\eta P(z)+\tfrac{1}{2\tau}\lVert x-z\rVert^{2}\ge v(z)+\eta P(z), so λ(v(z)+ηP(z))≤λw‾(x)\lambda(v(z)+\eta P(z))\le\lambda\underline{w}(x). (ii) As p=τ−1(x−z)p=\tau^{-1}(x-z), the monotonicity hypothesis and Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n give DP(x)⋅p−ξ⋅p=τ−1((DP(x)−ξ)⋅(x−z))≥0DP(x)\cdot p-\xi\cdot p=\tau^{-1}\bigl((DP(x)-\xi)\cdot(x-z)\bigr)\ge0, so ξ⋅p≤DP(x)⋅p\xi\cdot p\le DP(x)\cdot p. (iii) g(x)−g(z)≤∣g(x)−g(z)∣≤ρ(∥x−z∥)≤ρ(r(x))g(x)-g(z)\le|g(x)-g(z)|\le\rho(\lVert x-z\rVert)\le\rho(r(x)) by clause B1 and the monotonicity of ρ\rho, so g2(x)=g(x)−ηC−ρ(r(x))≤g(z)−ηCg_{2}(x)=g(x)-\eta C-\rho(r(x))\le g(z)-\eta C. Combining (i), (ii), (iii) with (11.2),

−F2(x,w‾(x),Dφ(x),D2φ(x))=g2(x)−λw‾(x)−θ22∥p∥2−DP(x)⋅p+κ2tr⁡X≤κ2n σ.-F_{2}\bigl(x,\underline{w}(x),D\varphi(x),D^{2}\varphi(x)\bigr)=g_{2}(x)-\lambda\underline{w}(x)-\tfrac{\theta_{2}}{2}\lVert p\rVert^{2}-DP(x)\cdot p+\tfrac{\kappa}{2}\operatorname{tr}X\le\tfrac{\kappa}{2}n\,\sigma .

As σ\sigma was an arbitrary positive number, (0.4) gives 0≤F2(x,w‾(x),Dφ(x),D2φ(x))0\le F_{2}(x,\underline{w}(x),D\varphi(x),D^{2}\varphi(x)). Since φ\varphi and xx were arbitrary and w‾\underline{w} is lower semicontinuous, w‾\underline{w} is a viscosity supersolution of F2F_{2} on DD by Viscosity Subsolution and Supersolution of a Second-Order Equation; this is clause B6.

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