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Proof of The Viscosity Sub- and Supersolution Properties are Local

lemmalem:viscosity-subsolution-local-2026a
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· 11,310 chars · 20 deps · depth 22 Reason: First publication of the proof: a test function on the open subset is replaced near the contact point by the quadratic of its second-order expansion shifted by a multiple of the identity, which is defined on the whole domain, and continuity of the operator removes the shift in the limit.

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 §matrices 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)=PRd_{\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 a0a\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 uVu|_{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:VR\varphi:V\to\mathbb{R} be of class C2C^{2} on VV and let x0Vx_{0}\in V be a point at which uVφu|_{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 FVF|_{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 εR\varepsilon\in\mathbb{R} be positive and put M=A+2εInS(n)M=A+2\varepsilon I_{n}\in\mathcal{S}(n). Let Q0:RnRQ_{0}:\mathbb{R}^{n}\to\mathbb{R} be given by Q0(w)=12w(Mw)+pw+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 wRnw\in\mathbb{R}^{n}. Let Q:RnRQ:\mathbb{R}^{n}\to\mathbb{R} be given by Q(z)=Q0(zx0)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(zx0)+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(x0x0)=Mx0Mx0=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 w0Rn=w(zz)=wzwz=0w\cdot 0_{\mathbb{R}^{n}}=w\cdot(z-z)=w\cdot z-w\cdot z=0 for all w,zRnw,z\in\mathbb{R}^{n}, by the part of claim 5 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n 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 δ1R\delta_{1}\in\mathbb{R} such that every hRnh\in\mathbb{R}^{n} with h<δ1\lVert h\rVert<\delta_{1} satisfies x0+hVx_{0}+h\in V and

φ(x0+h)φ(x0)ph12h(Ah)εh2.\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)+ph+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)+ph+12h(Ah)+εh2.\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 Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n 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)=2εh2h\cdot\bigl((2\varepsilon I_{n})h\bigr)=2\varepsilon\lVert h\rVert^{2}, whence 12h(Mh)=12h(Ah)+εh2\tfrac{1}{2}h\cdot(Mh)=\tfrac{1}{2}h\cdot(Ah)+\varepsilon\lVert h\rVert^{2}. Therefore

φ(x0+h)φ(x0)+ph+12h(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 δ2R\delta_{2}\in\mathbb{R} such that every yVy\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 δR\delta\in\mathbb{R} with δδ1\delta\le\delta_{1} and δδ2\delta\le\delta_{2}. Let yUy\in U satisfy dE(x0,y)<δd_{E}(x_{0},y)<\delta and put h=yx0h=y-x_{0}, so that y=x0+hy=x_{0}+h and, by claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n together with 1=1|-1|=1, h=yx0=x0y=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 yVy\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 CkC^k Map to an Open Subset the restriction QUQ|_{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(QU)(x0)=DQ(x0)=pD(Q|_{U})(x_{0})=DQ(x_{0})=p and D2(QU)(x0)=D2Q(x0)=MD^{2}(Q|_{U})(x_{0})=D^{2}Q(x_{0})=M. The displayed inequality says that uQUu-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 εR\varepsilon\in\mathbb{R}.

Passing to the limit. Let ηR\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 §at-point gives a positive δFR\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=12δF2\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}, pp=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)+ηη.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 §slack-above 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 uVu|_{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 uVφu|_{V}-\varphi having a local minimum at x0Vx_{0}\in V relative to VV, and keep the notation pp, AA. Run the argument above with M=A2εInM=A-2\varepsilon I_{n}: the same two-sided estimate, now used through the inequality φ(x0+h)φ(x0)ph12h(Ah)φ(x0+h)φ(x0)ph12h(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 uQUu-Q|_{U} has a local minimum at x0x_{0} relative to UU and 0F(x0,u(x0),p,A2εIn)0\le F(x_{0},u(x_{0}),p,A-2\varepsilon I_{n}) for every positive ε\varepsilon. Since dS(n)(A2εIn,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 §slack-below gives 0F(x0,u(x0),p,A)0\le F(x_{0},u(x_{0}),p,A).

Proof of claim 2. Assume that every xUx\in U has an open neighbourhood VV with xVUx\in V\subseteq U on which uVu|_{V} is a viscosity subsolution of FVF|_{V}.

Upper semicontinuity. Let xUx\in U and let VV be such a neighbourhood. Since VV is open, claim 4 of The Interior is the Largest Open Subset gives intRn(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 rRr\in\mathbb{R} with {zRn:dE(z,x)r}V\{z\in\mathbb{R}^{n}:d_{E}(z,x)\le r\}\subseteq V; in particular {zU:dE(z,x)r}V\{z\in U:d_{E}(z,x)\le r\}\subseteq V. The function uVu|_{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 xUx\in U was arbitrary, uu is upper semicontinuous on UU.

The test inequality. Let φ:UR\varphi:U\to\mathbb{R} be of class C2C^{2} on UU and let xUx\in U be a point at which uφu-\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 CkC^k Map to an Open Subset the restriction φV\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(φV)(x)=Dφ(x)D(\varphi|_{V})(x)=D\varphi(x) and D2(φV)(x)=D2φ(x)D^{2}(\varphi|_{V})(x)=D^{2}\varphi(x). Every yVy\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 uVφVu|_{V}-\varphi|_{V} has a local maximum at xx relative to VV. Since uVu|_{V} is a viscosity subsolution of FVF|_{V} on VV,

F(x,u(x),Dφ(x),D2φ(x))=FV(x,u(x),D(φV)(x),D2(φV)(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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