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Proof of The Test-Datum Estimate at a Maximum Point of the Doubled Function

lemmalem:doubled-test-estimate-hilbert-triple-2026a
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· 9,193 chars · 15 deps · depth 26 Reason: Initial publication of the proof: construction of the test functions and test data, verification of admissibility, and the chain of the three structural conditions.

Slicing the doubled function at the maximum point produces C2C^2 test functions for the subsolution and the supersolution; the resulting test data are shown to be R-bounded and admissible, the shift modulus moves both gradient arguments onto the common doubling gradient, the structure triple compares the two shifts there, and the properness constant converts the comparison into the asserted estimate.

Proof

Each result cited is universally quantified over the data in its own statement. Write Θ:V×VR\Theta:V\times V\to\mathbb{R} for the function in the hypothesis, so that Θ\Theta attains a maximum at (x^,y^)(\hat{x},\hat{y}).

Step 1 (test functions). Let φ:HR\varphi:H\to\mathbb{R} be given by φ(x)=α2xy^H2+p,xH\varphi(x)=\tfrac{\alpha}{2}|x-\hat{y}|_{H}^{2}+\langle p,x\rangle_{H}. By claims 3 and 1 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C2C^2 its two summands belong to C2(H)C^{2}(H), with gradients α(xy^)\alpha(x-\hat{y}) and pp and Hessians αIH\alpha I_{H} and 0Sym0_{\mathrm{Sym}} at every xHx\in H, so by Constants, Sums, Scalar Multiples and Differences of Differentiable Functions on an Open Subset of a Real Inner Product Space §sum φC2(H)\varphi\in C^{2}(H) with

Dφ(x^)=α(x^y^)+p,D2φ(x^)=αIH.D\varphi(\hat{x})=\alpha(\hat{x}-\hat{y})+p,\qquad D^{2}\varphi(\hat{x})=\alpha I_{H}.

Let ψ:HR\psi:H\to\mathbb{R} be given by ψ(y)=α2yx^H2q,yH\psi(y)=-\tfrac{\alpha}{2}|y-\hat{x}|_{H}^{2}-\langle q,y\rangle_{H}; by the same two lemmas together with Constants, Sums, Scalar Multiples and Differences of Differentiable Functions on an Open Subset of a Real Inner Product Space §scalar, ψC2(H)\psi\in C^{2}(H) with

Dψ(y^)=α(y^x^)q=α(x^y^)q,D2ψ(y^)=αIH.D\psi(\hat{y})=-\alpha(\hat{y}-\hat{x})-q=\alpha(\hat{x}-\hat{y})-q,\qquad D^{2}\psi(\hat{y})=-\alpha I_{H}.

For xVx\in V one has Θ(x,y^)=(uδ(x)φ(x))vδ+(y^)q,y^H\Theta(x,\hat{y})=\bigl(u^{-}_{\delta}(x)-\varphi(x)\bigr)-v^{+}_{\delta}(\hat{y})-\langle q,\hat{y}\rangle_{H}, and Θ(x,y^)Θ(x^,y^)\Theta(x,\hat{y})\le\Theta(\hat{x},\hat{y}); hence the function on VV with value uδ(x)φ(x)u^{-}_{\delta}(x)-\varphi(x) at xx satisfies

uδ(x)φ(x)uδ(x^)φ(x^)for every xV,u^{-}_{\delta}(x)-\varphi(x)\le u^{-}_{\delta}(\hat{x})-\varphi(\hat{x})\qquad\text{for every }x\in V,

and so has a local maximum relative to VV at x^\hat{x}, the condition of Local Maximum of a Function Relative to a Subset of a Metric Space holding with any positive radius. Likewise, for yVy\in V one has Θ(x^,y)=uδ(x^)p,x^H(vδ+(y)ψ(y))\Theta(\hat{x},y)=u^{-}_{\delta}(\hat{x})-\langle p,\hat{x}\rangle_{H}-\bigl(v^{+}_{\delta}(y)-\psi(y)\bigr), so the function with value vδ+(y)ψ(y)v^{+}_{\delta}(y)-\psi(y) at yy has a local minimum relative to VV at y^\hat{y}.

Step 2 (test data). Applying Viscosity Subsolution, Supersolution and Solution of a Second-Order Equation on a Hilbert Triple §subsolution with δ\delta, the test function φ\varphi, the point x^\hat{x} and the number ε\varepsilon yields x1D(A)x_{1}\in D(A), s1Rs_{1}\in\mathbb{R}, p1Hp_{1}\in H and X1Sym(H)X_{1}\in\mathrm{Sym}(H) with

x1x^H<ε,uδ(x1)uδ(x^)<ε,s1uδ(x^)<ε,p1Dφ(x^)H<ε,X1αIH<ε,|x_{1}-\hat{x}|_{H}<\varepsilon,\quad |u^{-}_{\delta}(x_{1})-u^{-}_{\delta}(\hat{x})|<\varepsilon,\quad |s_{1}-u^{-}_{\delta}(\hat{x})|<\varepsilon,\quad |p_{1}-D\varphi(\hat{x})|_{H}<\varepsilon,\quad \lVert X_{1}-\alpha I_{H}\rVert<\varepsilon,

and Fδ(x1,s1,p1,X1)εF^{-}_{\delta}(x_{1},s_{1},p_{1},X_{1})\le\varepsilon. Applying Viscosity Subsolution, Supersolution and Solution of a Second-Order Equation on a Hilbert Triple §supersolution with δ\delta, ψ\psi, y^\hat{y} and ε\varepsilon yields y1D(A)y_{1}\in D(A), t1Rt_{1}\in\mathbb{R}, q1Hq_{1}\in H and Y1Sym(H)Y_{1}\in\mathrm{Sym}(H) with

y1y^H<ε,vδ+(y1)vδ+(y^)<ε,t1vδ+(y^)<ε,q1Dψ(y^)H<ε,Y1+αIH<ε,|y_{1}-\hat{y}|_{H}<\varepsilon,\quad |v^{+}_{\delta}(y_{1})-v^{+}_{\delta}(\hat{y})|<\varepsilon,\quad |t_{1}-v^{+}_{\delta}(\hat{y})|<\varepsilon,\quad |q_{1}-D\psi(\hat{y})|_{H}<\varepsilon,\quad \lVert Y_{1}+\alpha I_{H}\rVert<\varepsilon,

and εFδ+(y1,t1,q1,Y1)-\varepsilon\le F^{+}_{\delta}(y_{1},t_{1},q_{1},Y_{1}).

Step 3 (the data are admissible). By Basic Properties of the δ\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity §bound, uδ(x1)Cδh(x1)u^{-}_{\delta}(x_{1})\le C-\delta h(x_{1}), so, using CBC\le B, uδ(x^)B-u^{-}_{\delta}(\hat{x})\le B and ε1\varepsilon\le1,

δh(x1)Cuδ(x1)Cuδ(x^)+ε2B+1,\delta h(x_{1})\le C-u^{-}_{\delta}(x_{1})\le C-u^{-}_{\delta}(\hat{x})+\varepsilon\le 2B+1 ,

whence h(x1)2B+1δ<Rh(x_{1})\le\frac{2B+1}{\delta}<R. By the same claim C+δh(y1)vδ+(y1)-C+\delta h(y_{1})\le v^{+}_{\delta}(y_{1}), so δh(y1)vδ+(y1)+Cvδ+(y^)+ε+C2B+1\delta h(y_{1})\le v^{+}_{\delta}(y_{1})+C\le v^{+}_{\delta}(\hat{y})+\varepsilon+C\le2B+1 and h(y1)<Rh(y_{1})<R. Next s1uδ(x^)+εB+1<R|s_{1}|\le|u^{-}_{\delta}(\hat{x})|+\varepsilon\le B+1<R and t1B+1<R|t_{1}|\le B+1<R, because B+13B+2<RB+1\le3B+2<R and 0B0\le B.

Since IH(x,y)=x,yHxHyH|I_{H}(x,y)|=|\langle x,y\rangle_{H}|\le|x|_{H}|y|_{H} for x,yHx,y\in H by The Cauchy-Schwarz Inequality in a Real Inner Product Space, claim 2 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity gives IH1\lVert I_{H}\rVert\le1, and hence αIHα\lVert\alpha I_{H}\rVert\le\alpha and αIHα\lVert-\alpha I_{H}\rVert\le\alpha by the homogeneity of the norm in Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity §norm-axioms. Therefore, by the triangle inequality of that same claim,

X1αIH+X1αIHα+1<R,Y1α+1<R.\lVert X_{1}\rVert\le\lVert\alpha I_{H}\rVert+\lVert X_{1}-\alpha I_{H}\rVert\le\alpha+1<R,\qquad \lVert Y_{1}\rVert\le\alpha+1<R .

Finally, by The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle,

p1HDφ(x^)H+εαx^y^H+pH+εG+σ+εG+2<G+2α<R,|p_{1}|_{H}\le|D\varphi(\hat{x})|_{H}+\varepsilon\le\alpha|\hat{x}-\hat{y}|_{H}+|p|_{H}+\varepsilon\le G+\sigma+\varepsilon\le G+2<G+2\alpha<R,

using 1<α1<\alpha, and likewise q1HG+2<R|q_{1}|_{H}\le G+2<R. Thus ξ1=(x1,s1,p1,X1)\xi_{1}=(x_{1},s_{1},p_{1},X_{1}) and η1=(y1,t1,q1,Y1)\eta_{1}=(y_{1},t_{1},q_{1},Y_{1}) are RR-bounded test data, and

Fδ(ξ1)Fδ+(η1)ε+ε2<α+1<R.F^{-}_{\delta}(\xi_{1})-F^{+}_{\delta}(\eta_{1})\le\varepsilon+\varepsilon\le2<\alpha+1<R .

Hence ξ1Sδ,R\xi_{1}\in S^{-}_{\delta,R} and η1Sδ,R+\eta_{1}\in S^{+}_{\delta,R} by Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets §admissible, each datum serving as the witness required for the other.

Step 4 (moving the gradient arguments). Put P=α(x1y1)P=\alpha(x_{1}-y_{1}), τ1=Pp1H\tau_{1}=|P-p_{1}|_{H} and τ2=Pq1H\tau_{2}=|P-q_{1}|_{H}; these are nonnegative. By the triangle inequality,

τ1α(x1y1)(x^y^)H+α(x^y^)+pp1H+pHα(ε+ε)+ε+σ=(2α+1)ε+σ,\tau_{1}\le\alpha\bigl|(x_{1}-y_{1})-(\hat{x}-\hat{y})\bigr|_{H}+\bigl|\alpha(\hat{x}-\hat{y})+p-p_{1}\bigr|_{H}+|p|_{H}\le\alpha(\varepsilon+\varepsilon)+\varepsilon+\sigma=(2\alpha+1)\varepsilon+\sigma ,

and the same bound holds for τ2\tau_{2}, since Dψ(y^)=α(x^y^)qD\psi(\hat{y})=\alpha(\hat{x}-\hat{y})-q and qHσ|q|_{H}\le\sigma.

Apply the first condition of The Shift-Continuity Condition on Admissible Test Data §modulus to ξ1\xi_{1} with the perturbations Pp1HP-p_{1}\in H and 0SymSym(H)0_{\mathrm{Sym}}\in\mathrm{Sym}(H): since p1+(Pp1)=Pp_{1}+(P-p_{1})=P, X1+0Sym=X1X_{1}+0_{\mathrm{Sym}}=X_{1} and 0Sym=0\lVert 0_{\mathrm{Sym}}\rVert=0,

Fδ(x1,s1,P,X1)Fδ(x1,s1,p1,X1)+ω(τ1)ε+ω(τ1).F^{-}_{\delta}(x_{1},s_{1},P,X_{1})\le F^{-}_{\delta}(x_{1},s_{1},p_{1},X_{1})+\omega(\tau_{1})\le\varepsilon+\omega(\tau_{1}).

Apply the second condition to η1\eta_{1} with the perturbations Pq1P-q_{1} and 0Sym0_{\mathrm{Sym}}:

εω(τ2)Fδ+(y1,t1,q1,Y1)ω(τ2)Fδ+(y1,t1,P,Y1).-\varepsilon-\omega(\tau_{2})\le F^{+}_{\delta}(y_{1},t_{1},q_{1},Y_{1})-\omega(\tau_{2})\le F^{+}_{\delta}(y_{1},t_{1},P,Y_{1}).

Step 5 (the structure condition). We have x1,y1D(A)=Wx_{1},y_{1}\in D(A)=W, t1B+13B+2|t_{1}|\le B+1\le3B+2, 1<α1<\alpha, 0<δ<10<\delta<1 and P=α(x1y1)P=\alpha(x_{1}-y_{1}), so The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple §triple, applied to the structure triple (ω1,ω2,ω3)(\omega_{1},\omega_{2},\omega_{3}) at 3B+23B+2 with the value argument t1t_{1} and the form arguments X1X_{1} and Y1Y_{1}, gives

Fδ+(y1,t1,P,Y1)ω1(x1y1H)ω2(αx1y1H2)ω3(δα2x1y1H2)  Fδ(x1,t1,P,X1).F^{+}_{\delta}(y_{1},t_{1},P,Y_{1})-\omega_{1}\bigl(|x_{1}-y_{1}|_{H}\bigr)-\omega_{2}\bigl(\alpha|x_{1}-y_{1}|_{H}^{2}\bigr)-\omega_{3}\bigl(\delta\alpha^{2}|x_{1}-y_{1}|_{H}^{2}\bigr)\ \le\ F^{-}_{\delta}(x_{1},t_{1},P,X_{1}).

Step 6 (properness and conclusion). Since s1uδ(x^)<ε|s_{1}-u^{-}_{\delta}(\hat{x})|<\varepsilon and t1vδ+(y^)<ε|t_{1}-v^{+}_{\delta}(\hat{y})|<\varepsilon,

uδ(x^)vδ+(y^)(s1+ε)(t1ε)=s1t1+2ε.()u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\le(s_{1}+\varepsilon)-(t_{1}-\varepsilon)=s_{1}-t_{1}+2\varepsilon . \tag{$*$}

Suppose first that t1s1t_{1}\le s_{1}. By Step 3 we have 0δh(x1)2B+10\le\delta h(x_{1})\le2B+1, s1B+1|s_{1}|\le B+1 and t1B+1|t_{1}|\le B+1, so both s1+δh(x1)s_{1}+\delta h(x_{1}) and t1+δh(x1)t_{1}+\delta h(x_{1}) lie between (3B+2)-(3B+2) and 3B+23B+2, and t1+δh(x1)s1+δh(x1)t_{1}+\delta h(x_{1})\le s_{1}+\delta h(x_{1}). Applying Locally Strictly Proper Second-Order Equation Operator on a Hilbert Triple §constant at the level 3B+23B+2, with the point x1x_{1}, the gradient argument P+δAx1HP+\delta Ax_{1}\in H and the form argument X1V+δIVSym(V)X_{1}|_{V}+\delta I_{V}\in\mathrm{Sym}(V), and reading the two resulting values of FF through Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts §shifted, we obtain

λ(s1t1)=λ((s1+δh(x1))(t1+δh(x1)))Fδ(x1,s1,P,X1)Fδ(x1,t1,P,X1).\lambda(s_{1}-t_{1})=\lambda\bigl((s_{1}+\delta h(x_{1}))-(t_{1}+\delta h(x_{1}))\bigr)\le F^{-}_{\delta}(x_{1},s_{1},P,X_{1})-F^{-}_{\delta}(x_{1},t_{1},P,X_{1}).

Combining this with Steps 4 and 5,

λ(s1t1)ε+ω(τ1)Fδ+(y1,t1,P,Y1)+ω1(x1y1H)+ω2(αx1y1H2)+ω3(δα2x1y1H2)\lambda(s_{1}-t_{1})\le\varepsilon+\omega(\tau_{1})-F^{+}_{\delta}(y_{1},t_{1},P,Y_{1})+\omega_{1}\bigl(|x_{1}-y_{1}|_{H}\bigr)+\omega_{2}\bigl(\alpha|x_{1}-y_{1}|_{H}^{2}\bigr)+\omega_{3}\bigl(\delta\alpha^{2}|x_{1}-y_{1}|_{H}^{2}\bigr)  2ε+ω(τ1)+ω(τ2)+ω1(x1y1H)+ω2(αx1y1H2)+ω3(δα2x1y1H2).\le\ 2\varepsilon+\omega(\tau_{1})+\omega(\tau_{2})+\omega_{1}\bigl(|x_{1}-y_{1}|_{H}\bigr)+\omega_{2}\bigl(\alpha|x_{1}-y_{1}|_{H}^{2}\bigr)+\omega_{3}\bigl(\delta\alpha^{2}|x_{1}-y_{1}|_{H}^{2}\bigr).

Multiplying ()(*) by the positive number λ\lambda and adding 2λε2\lambda\varepsilon to the previous display gives the asserted estimate.

Suppose now that s1<t1s_{1}<t_{1}. Then ()(*) gives uδ(x^)vδ+(y^)<2εu^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})<2\varepsilon, so λ(uδ(x^)vδ+(y^))<2λε\lambda\bigl(u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\bigr)<2\lambda\varepsilon, and the asserted estimate holds because its remaining right-hand terms are nonnegative: the values of the moduli of continuity ω\omega, ω1\omega_{1}, ω2\omega_{2}, ω3\omega_{3} are nonnegative by clause 1 of Modulus of Continuity, and 0<2ε0<2\varepsilon.

In both cases x1,y1D(A)x_{1},y_{1}\in D(A) satisfy x1x^H<ε|x_{1}-\hat{x}|_{H}<\varepsilon and y1y^H<ε|y_{1}-\hat{y}|_{H}<\varepsilon by Step 2, and τ1,τ2\tau_{1},\tau_{2} satisfy the stated bounds by Step 4.

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