TheoremBase

The two-element family is locally uniformly bounded above because each member is upper semicontinuous, its pointwise supremum is the pointwise maximum, and that maximum is upper semicontinuous, hence equal to its own upper semicontinuous envelope.

Proof

Conventions. 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 being an axiom of the ordered field R\mathbb{R}. A strict inequality a<ba<b implies a≤ba\le b by the definition of the strict order.

Proof. Put F={u,v}\mathcal{F}=\{u,v\}, a nonempty set of viscosity subsolutions of FF on UU.

The family is locally uniformly bounded above. Let x∈Ux\in U. Being viscosity subsolutions, uu and vv are upper semicontinuous on UU, so, applying upper semicontinuity at xx with the positive real 11, which is positive by claim 6 of Elementary Order Arithmetic in an Ordered Field, there are positive δu,δv∈R\delta_{u},\delta_{v}\in\mathbb{R} such that every y∈Uy\in U with dE(x,y)<δud_{E}(x,y)<\delta_{u} satisfies u(y)<u(x)+1u(y)<u(x)+1 and every y∈Uy\in U with dE(x,y)<δvd_{E}(x,y)<\delta_{v} satisfies v(y)<v(x)+1v(y)<v(x)+1. By claim 9 of Elementary Order Arithmetic in an Ordered Field there is a positive δ\delta with δ≤δu\delta\le\delta_{u} and δ≤δv\delta\le\delta_{v}, and by claim 8 of that lemma the real number r=δ2r=\tfrac{\delta}{2} is positive and satisfies r<δr<\delta. Put c=max⁡{u(x),v(x)}+1c=\max\{u(x),v(x)\}+1. Let y∈Uy\in U satisfy dE(y,x)≤rd_{E}(y,x)\le r. Then dE(x,y)=dE(y,x)≤r<δd_{E}(x,y)=d_{E}(y,x)\le r<\delta by the symmetry axiom of a metric, so dE(x,y)<δud_{E}(x,y)<\delta_{u} and dE(x,y)<δvd_{E}(x,y)<\delta_{v} by the mixed transitivity of claim 2 of Elementary Order Arithmetic in an Ordered Field; hence u(y)<u(x)+1≤cu(y)<u(x)+1\le c and v(y)<v(x)+1≤cv(y)<v(x)+1\le c by claim 1 of Elementary Properties of the Maximum of Two Elements and the compatibility of ≤\le with addition. Thus every member of F\mathcal{F} is at most cc at every such yy.

The supremum is the maximum. Let w:U→Rw:U\to\mathbb{R} be the pointwise supremum of F\mathcal{F} formed in The Upper Semicontinuous Envelope of a Supremum of Viscosity Subsolutions is a Viscosity Subsolution. For x∈Ux\in U the set of values is {u(x),v(x)}\{u(x),v(x)\}; by claim 1 of Elementary Properties of the Maximum of Two Elements the number max⁡{u(x),v(x)}\max\{u(x),v(x)\} is an upper bound of it, and by claim 3 of that lemma every upper bound c′c' of it satisfies max⁡{u(x),v(x)}≤c′\max\{u(x),v(x)\}\le c'. Hence max⁡{u(x),v(x)}\max\{u(x),v(x)\} is the least upper bound, that is w(x)=(u∨v)(x)w(x)=(u\vee v)(x).

Conclusion. By claim 2 of The Maximum of Two Upper Semicontinuous Functions the function u∨vu\vee v is upper semicontinuous on UU, so ww is, and claim 4 of Properties of the Upper Semicontinuous Envelope gives w∗(x)=w(x)w^{*}(x)=w(x) for every x∈Ux\in U; that is, w∗=u∨vw^{*}=u\vee v. By The Upper Semicontinuous Envelope of a Supremum of Viscosity Subsolutions is a Viscosity Subsolution the function w∗w^{*} is a viscosity subsolution of FF on UU, and therefore so is u∨vu\vee v. ■\blacksquare

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