TheoremBase

For the restriction, a test function on the open subset is replaced near the point by the quadratic built from its second-order expansion with an extra multiple of the identity, which is defined on all of the larger domain; continuity of the operator then lets the extra multiple tend to zero. The converse direction only restricts a test function, since a local maximum relative to the larger set is one relative to the smaller.

Proof

Conventions. From the setting we use the real numbers and their order, Euclidean space with its sum, difference, dot product, norm and distance dEd_{E}, the set S(n)\mathcal{S}(n) with its norm and distance dS(n)d_{\mathcal{S}(n)}, the identity matrix InI_{n} and the matrix-vector product, and the notions of class C2C^{2}, gradient, Hessian, semicontinuity and local extrema. Recall from clause Second-Order Equations on Euclidean Open Sets (iii) that S(n)\mathcal{S}(n) contains aInaI_{n} for every real aa and is closed under sums and differences, and that dS(n)(P,R)=∥P−R∥d_{\mathcal{S}(n)}(P,R)=\lVert P-R\rVert. We write 2ε2\varepsilon for ε+ε\varepsilon+\varepsilon. Elementary order facts are those of Elementary Order Arithmetic in an Ordered Field, whose claim 1 is the compatibility of the strict order with addition, the non-strict law and the transitivity of ≤\le being axioms of the ordered field R\mathbb{R}. We use twice that ∣a∣=a|a|=a for a positive real aa: by claim 1 of Properties of the Absolute Value in an Ordered Field the number ∣a∣|a| is nonnegative and equals aa or −a-a, and in the second case −a-a would be nonnegative, hence a≤0a\le 0 by claim 4 of Elementary Order Arithmetic in an Ordered Field, contrary to the positivity of aa. In particular ∣1∣=1|1|=1, since 0<10<1 by claim 6 of Elementary Order Arithmetic in an Ordered Field, and therefore ∣−1∣=∣1∣=1|-1|=|1|=1 by claim 2 of Properties of the Absolute Value in an Ordered Field.

Proof of claim 1. We give the argument for subsolutions and indicate at the end the changes for supersolutions.

Being a viscosity subsolution of FF on UU, the function uu is upper semicontinuous on UU; hence u∣Vu|_{V} is upper semicontinuous on VV by claim 2 of Negation, Restriction, and Separated Differences of Semicontinuous Functions, applied at each point of VV.

Let φ:V→R\varphi:V\to\mathbb{R} be of class C2C^{2} on VV and let x0∈Vx_{0}\in V be a point at which u∣V−φu|_{V}-\varphi has a local maximum relative to VV. Write p=Dφ(x0)p=D\varphi(x_{0}) and A=D2φ(x0)∈S(n)A=D^{2}\varphi(x_{0})\in\mathcal{S}(n). Since F∣VF|_{V} agrees with FF at quadruples with first entry in VV, it suffices to prove that F(x0,u(x0),p,A)≤0F(x_{0},u(x_{0}),p,A)\le 0.

A quadratic majorant. Let ε∈R\varepsilon\in\mathbb{R} be positive and put M=A+2εIn∈S(n)M=A+2\varepsilon I_{n}\in\mathcal{S}(n). Let Q0:Rn→RQ_{0}:\mathbb{R}^{n}\to\mathbb{R} be given by Q0(w)=12 w⋅(Mw)+p⋅w+φ(x0)Q_{0}(w)=\tfrac{1}{2}\,w\cdot(Mw)+p\cdot w+\varphi(x_{0}), which by claim 1 of Quadratic and Affine Functions of Class C2C^2, Translation, and Quadratic Perturbation of Semiconvexity is of class C2C^{2} on Rn\mathbb{R}^{n} with DQ0(w)=Mw+pDQ_{0}(w)=Mw+p and D2Q0(w)=MD^{2}Q_{0}(w)=M for every w∈Rnw\in\mathbb{R}^{n}. Let Q:Rn→RQ:\mathbb{R}^{n}\to\mathbb{R} be given by Q(z)=Q0(z−x0)Q(z)=Q_{0}(z-x_{0}); by claim 2 of Quadratic and Affine Functions of Class C2C^2, Translation, and Quadratic Perturbation of Semiconvexity, applied to Q0Q_{0} on the open set Rn\mathbb{R}^{n} with the translation vector −x0-x_{0}, the function QQ is of class C2C^{2} on Rn\mathbb{R}^{n} with DQ(z)=M(z−x0)+pDQ(z)=M(z-x_{0})+p and D2Q(z)=MD^{2}Q(z)=M. In particular DQ(x0)=pDQ(x_{0})=p and D2Q(x0)=MD^{2}Q(x_{0})=M, since M(x0−x0)=Mx0−Mx0=0RnM(x_{0}-x_{0})=Mx_{0}-Mx_{0}=0_{\mathbb{R}^{n}} by claim 3 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum; and Q(x0)=Q0(0Rn)=φ(x0)Q(x_{0})=Q_{0}(0_{\mathbb{R}^{n}})=\varphi(x_{0}), because w⋅0Rn=w⋅(z−z)=w⋅z−w⋅z=0w\cdot 0_{\mathbb{R}^{n}}=w\cdot(z-z)=w\cdot z-w\cdot z=0 for all w,z∈Rnw,z\in\mathbb{R}^{n}, by the part of claim 5 of The Dot Product on Rn\mathbb{R}^n Is Symmetric, Bilinear and Positive Definite concerning differences in the second argument.

By claim 2 of Basic Properties of Twice Differentiability at a Point the function φ\varphi is twice differentiable at x0x_{0} with first-order coefficient pp and Hessian AA. Applying that definition with the positive real ε\varepsilon gives a positive δ1∈R\delta_{1}\in\mathbb{R} such that every h∈Rnh\in\mathbb{R}^{n} with ∥h∥<δ1\lVert h\rVert<\delta_{1} satisfies x0+h∈Vx_{0}+h\in V and

∣φ(x0+h)−φ(x0)−p⋅h−12 h⋅(Ah)∣≤ε∥h∥2.\bigl|\varphi(x_{0}+h)-\varphi(x_{0})-p\cdot h-\tfrac{1}{2}\,h\cdot(Ah)\bigr|\le\varepsilon\lVert h\rVert^{2}.

By claim 3 of Properties of the Absolute Value in an Ordered Field a real number is at most its own absolute value, so adding φ(x0)+p⋅h+12h⋅(Ah)\varphi(x_{0})+p\cdot h+\tfrac{1}{2}h\cdot(Ah) to both sides of the resulting inequality gives

φ(x0+h)≤φ(x0)+p⋅h+12 h⋅(Ah)+ε∥h∥2.\varphi(x_{0}+h)\le\varphi(x_{0})+p\cdot h+\tfrac{1}{2}\,h\cdot(Ah)+\varepsilon\lVert h\rVert^{2}.

On the other hand claim 1 of Linearity of the Matrix-Vector Product and the Quadratic Form as a Double Sum gives Mh=Ah+(2εIn)hMh=Ah+(2\varepsilon I_{n})h, claim 5 of The Dot Product on Rn\mathbb{R}^n Is Symmetric, Bilinear and Positive Definite gives h⋅(Mh)=h⋅(Ah)+h⋅((2εIn)h)h\cdot(Mh)=h\cdot(Ah)+h\cdot\bigl((2\varepsilon I_{n})h\bigr), and claim 6 of Vector, Entry and Comparison Bounds for the Norm of a Symmetric Real Matrix gives h⋅((2εIn)h)=2ε∥h∥2h\cdot\bigl((2\varepsilon I_{n})h\bigr)=2\varepsilon\lVert h\rVert^{2}, whence 12h⋅(Mh)=12h⋅(Ah)+ε∥h∥2\tfrac{1}{2}h\cdot(Mh)=\tfrac{1}{2}h\cdot(Ah)+\varepsilon\lVert h\rVert^{2}. Therefore

φ(x0+h)≤φ(x0)+p⋅h+12 h⋅(Mh)=Q0(h)=Q(x0+h)whenever ∥h∥<δ1.\varphi(x_{0}+h)\le\varphi(x_{0})+p\cdot h+\tfrac{1}{2}\,h\cdot(Mh)=Q_{0}(h)=Q(x_{0}+h)\qquad\text{whenever }\lVert h\rVert<\delta_{1}.

Transfer of the maximum. By the definition of a local maximum relative to VV there is a positive δ2∈R\delta_{2}\in\mathbb{R} such that every y∈Vy\in V with dE(x0,y)<δ2d_{E}(x_{0},y)<\delta_{2} satisfies u(y)−φ(y)≤u(x0)−φ(x0)u(y)-\varphi(y)\le u(x_{0})-\varphi(x_{0}). By claim 9 of Elementary Order Arithmetic in an Ordered Field there is a positive δ∈R\delta\in\mathbb{R} with δ≤δ1\delta\le\delta_{1} and δ≤δ2\delta\le\delta_{2}. Let y∈Uy\in U satisfy dE(x0,y)<δd_{E}(x_{0},y)<\delta and put h=y−x0h=y-x_{0}, so that y=x0+hy=x_{0}+h and, by claim 5 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square together with ∣−1∣=1|-1|=1, ∥h∥=∥y−x0∥=∥x0−y∥=dE(x0,y)<δ\lVert h\rVert=\lVert y-x_{0}\rVert=\lVert x_{0}-y\rVert=d_{E}(x_{0},y)<\delta. By the mixed transitivity of claim 2 of Elementary Order Arithmetic in an Ordered Field we get ∥h∥<δ1\lVert h\rVert<\delta_{1} and dE(x0,y)<δ2d_{E}(x_{0},y)<\delta_{2}; hence y∈Vy\in V, φ(y)≤Q(y)\varphi(y)\le Q(y) and u(y)−φ(y)≤u(x0)−φ(x0)u(y)-\varphi(y)\le u(x_{0})-\varphi(x_{0}), so

u(y)−Q(y)≤u(y)−φ(y)≤u(x0)−φ(x0)=u(x0)−Q(x0).u(y)-Q(y)\le u(y)-\varphi(y)\le u(x_{0})-\varphi(x_{0})=u(x_{0})-Q(x_{0}).

By claim 3 of Restriction of a Cᵏ Function to an Open Subset the restriction Q∣UQ|_{U} is of class C2C^{2} on UU, and by claim 1 of that lemma, applied to QQ and to its first partial derivatives, D(Q∣U)(x0)=DQ(x0)=pD(Q|_{U})(x_{0})=DQ(x_{0})=p and D2(Q∣U)(x0)=D2Q(x0)=MD^{2}(Q|_{U})(x_{0})=D^{2}Q(x_{0})=M. The displayed inequality says that u−Q∣Uu-Q|_{U} has a local maximum at x0x_{0} relative to UU, so, uu being a viscosity subsolution of FF on UU,

F(x0,u(x0),p,A+2εIn)≤0.F\bigl(x_{0},u(x_{0}),p,A+2\varepsilon I_{n}\bigr)\le 0 .

This holds for every positive ε∈R\varepsilon\in\mathbb{R}.

Passing to the limit. Let η∈R\eta\in\mathbb{R} be positive. Since FF is continuous it is continuous at (x0,u(x0),p,A)(x_{0},u(x_{0}),p,A), so clause Continuity of a Second-Order Equation Operator (i) gives a positive δF∈R\delta_{F}\in\mathbb{R} such that every quadruple whose four displayed distances to (x0,u(x0),p,A)(x_{0},u(x_{0}),p,A) are smaller than δF\delta_{F} has FF-value within η\eta of F(x0,u(x0),p,A)F(x_{0},u(x_{0}),p,A). By claim 8 of Elementary Order Arithmetic in an Ordered Field the real number δF2\tfrac{\delta_{F}}{2} is positive and smaller than δF\delta_{F}, and ε=12⋅δF2\varepsilon=\tfrac{1}{2}\cdot\tfrac{\delta_{F}}{2} is positive with 2ε=δF2<δF2\varepsilon=\tfrac{\delta_{F}}{2}<\delta_{F}. For this ε\varepsilon the quadruple (x0,u(x0),p,A+2εIn)(x_{0},u(x_{0}),p,A+2\varepsilon I_{n}) satisfies dE(x0,x0)=0<δFd_{E}(x_{0},x_{0})=0<\delta_{F}, ∣u(x0)−u(x0)∣=0<δF|u(x_{0})-u(x_{0})|=0<\delta_{F}, ∥p−p∥=0<δF\lVert p-p\rVert=0<\delta_{F} and, by claim 6 of Vector, Entry and Comparison Bounds for the Norm of a Symmetric Real Matrix,

dS(n)(A+2εIn,A)=∥2εIn∥=∣2ε∣=2ε<δF.d_{\mathcal{S}(n)}\bigl(A+2\varepsilon I_{n},A\bigr)=\lVert 2\varepsilon I_{n}\rVert=|2\varepsilon|=2\varepsilon<\delta_{F}.

Hence ∣F(x0,u(x0),p,A+2εIn)−F(x0,u(x0),p,A)∣<η\bigl|F(x_{0},u(x_{0}),p,A+2\varepsilon I_{n})-F(x_{0},u(x_{0}),p,A)\bigr|<\eta, and claim 3 of Properties of the Absolute Value in an Ordered Field gives

F(x0,u(x0),p,A)≤F(x0,u(x0),p,A+2εIn)+η≤η.F(x_{0},u(x_{0}),p,A)\le F\bigl(x_{0},u(x_{0}),p,A+2\varepsilon I_{n}\bigr)+\eta\le\eta .

As η\eta was an arbitrary positive real, Comparison of Real Numbers with Arbitrary Positive Slack (i) gives F(x0,u(x0),p,A)≤0F(x_{0},u(x_{0}),p,A)\le 0, which is what had to be shown.

Supersolutions. Suppose uu is a viscosity supersolution of FF on UU. Then u∣Vu|_{V} is lower semicontinuous on VV by claim 2 of Negation, Restriction, and Separated Differences of Semicontinuous Functions. Let φ\varphi be of class C2C^{2} on VV with u∣V−φu|_{V}-\varphi having a local minimum at x0∈Vx_{0}\in V relative to VV, and keep the notation pp, AA. Run the argument above with M=A−2εInM=A-2\varepsilon I_{n}: the same two-sided estimate, now used through the inequality −∣φ(x0+h)−φ(x0)−p⋅h−12h⋅(Ah)∣≤φ(x0+h)−φ(x0)−p⋅h−12h⋅(Ah)-\bigl|\varphi(x_{0}+h)-\varphi(x_{0})-p\cdot h-\tfrac{1}{2}h\cdot(Ah)\bigr|\le\varphi(x_{0}+h)-\varphi(x_{0})-p\cdot h-\tfrac{1}{2}h\cdot(Ah) of claim 3 of Properties of the Absolute Value in an Ordered Field, gives Q(x0+h)≤φ(x0+h)Q(x_{0}+h)\le\varphi(x_{0}+h) whenever ∥h∥<δ1\lVert h\rVert<\delta_{1}, so that u−Q∣Uu-Q|_{U} has a local minimum at x0x_{0} relative to UU and 0≤F(x0,u(x0),p,A−2εIn)0\le F(x_{0},u(x_{0}),p,A-2\varepsilon I_{n}) for every positive ε\varepsilon. Since dS(n)(A−2εIn,A)=∥−2εIn∥=∣−2ε∣=2εd_{\mathcal{S}(n)}(A-2\varepsilon I_{n},A)=\lVert -2\varepsilon I_{n}\rVert=|-2\varepsilon|=2\varepsilon by claim 6 of Vector, Entry and Comparison Bounds for the Norm of a Symmetric Real Matrix and claim 2 of Properties of the Absolute Value in an Ordered Field, the same limiting argument together with Comparison of Real Numbers with Arbitrary Positive Slack (ii) gives 0≤F(x0,u(x0),p,A)0\le F(x_{0},u(x_{0}),p,A).

Proof of claim 2. Assume that every x∈Ux\in U has an open neighbourhood VV with x∈V⊆Ux\in V\subseteq U on which u∣Vu|_{V} is a viscosity subsolution of F∣VF|_{V}.

Upper semicontinuity. Let x∈Ux\in U and let VV be such a neighbourhood. Since VV is open, claim 4 of The Interior is the Largest Open Subset gives int⁡Rn(V)=V\operatorname{int}_{\mathbb{R}^{n}}(V)=V, so claim 1 of Interior Points in the Metric Topology are Exactly the Centres of Contained Closed Balls provides a positive r∈Rr\in\mathbb{R} with {z∈Rn:dE(z,x)≤r}⊆V\{z\in\mathbb{R}^{n}:d_{E}(z,x)\le r\}\subseteq V; in particular {z∈U:dE(z,x)≤r}⊆V\{z\in U:d_{E}(z,x)\le r\}\subseteq V. The function u∣Vu|_{V} is upper semicontinuous on VV, in particular at xx relative to VV, so claim 3 of Semicontinuity and the Semicontinuous Envelopes are Local Notions, applied with UU in the role of the ambient subset and this rr, shows that uu is upper semicontinuous at xx relative to UU. As x∈Ux\in U was arbitrary, uu is upper semicontinuous on UU.

The test inequality. Let φ:U→R\varphi:U\to\mathbb{R} be of class C2C^{2} on UU and let x∈Ux\in U be a point at which u−φu-\varphi has a local maximum relative to UU, with modulus δ\delta. Let VV be a neighbourhood of xx as above. By claim 3 of Restriction of a Cᵏ Function to an Open Subset the restriction φ∣V\varphi|_{V} is of class C2C^{2} on VV, and by claim 1 of that lemma, applied to φ\varphi and to its first partial derivatives, D(φ∣V)(x)=Dφ(x)D(\varphi|_{V})(x)=D\varphi(x) and D2(φ∣V)(x)=D2φ(x)D^{2}(\varphi|_{V})(x)=D^{2}\varphi(x). Every y∈Vy\in V with dE(x,y)<δd_{E}(x,y)<\delta lies in UU, so u(y)−φ(y)≤u(x)−φ(x)u(y)-\varphi(y)\le u(x)-\varphi(x); hence u∣V−φ∣Vu|_{V}-\varphi|_{V} has a local maximum at xx relative to VV. Since u∣Vu|_{V} is a viscosity subsolution of F∣VF|_{V} on VV,

F(x,u(x),Dφ(x),D2φ(x))=F∣V(x,u(x),D(φ∣V)(x),D2(φ∣V)(x))≤0.F\bigl(x,u(x),D\varphi(x),D^{2}\varphi(x)\bigr)=F|_{V}\bigl(x,u(x),D(\varphi|_{V})(x),D^{2}(\varphi|_{V})(x)\bigr)\le 0 .

Thus uu is a viscosity subsolution of FF on UU. The supersolution case is identical, with lower semicontinuity in place of upper semicontinuity, local minima in place of local maxima, and the inequality reversed. ■\blacksquare

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