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

lemmalem:doubled-test-estimate-hilbert-triple-2026b
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Β· 9,343 chars Β· 15 deps Β· depth 26 Reason: Copied from the previous proof version; Steps 5-6 adapted to the structure-pair form of (F2).

Quadratic test functions are read off the doubled maximum, the viscosity definitions supply admissible test data near the maximum point, the shift modulus moves the gradient arguments to alpha(x1 - y1), and the structure pair and properness give the estimate.

Proof

Each result cited is universally quantified over the data in its own statement. Write Θ:VΓ—Vβ†’R\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 Ο†:Hβ†’R\varphi:H\to\mathbb{R} be given by Ο†(x)=Ξ±2∣xβˆ’y^∣H2+⟨p,x⟩H\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 Ξ±(xβˆ’y^)\alpha(x-\hat{y}) and pp and Hessians Ξ±IH\alpha I_{H} and 0Sym0_{\mathrm{Sym}} at every x∈Hx\in H, so by Constants, Sums, Scalar Multiples and Differences of Differentiable Functions on an Open Subset of a Real Inner Product Space Β§sum Ο†βˆˆC2(H)\varphi\in C^{2}(H) with

DΟ†(x^)=Ξ±(x^βˆ’y^)+p,D2Ο†(x^)=Ξ±IH.D\varphi(\hat{x})=\alpha(\hat{x}-\hat{y})+p,\qquad D^{2}\varphi(\hat{x})=\alpha I_{H}.

Let ψ:Hβ†’R\psi:H\to\mathbb{R} be given by ψ(y)=βˆ’Ξ±2∣yβˆ’x^∣H2βˆ’βŸ¨q,y⟩H\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 Β§scalar, ψ∈C2(H)\psi\in C^{2}(H) with

Dψ(y^)=βˆ’Ξ±(y^βˆ’x^)βˆ’q=Ξ±(x^βˆ’y^)βˆ’q,D2ψ(y^)=βˆ’Ξ±IH.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 x∈Vx\in V one has Θ(x,y^)=(uΞ΄βˆ’(x)βˆ’Ο†(x))βˆ’vΞ΄+(y^)βˆ’βŸ¨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^)β‰€Ξ˜(x^,y^)\Theta(x,\hat{y})\le\Theta(\hat{x},\hat{y}); hence the function on VV with value uΞ΄βˆ’(x)βˆ’Ο†(x)u^{-}_{\delta}(x)-\varphi(x) at xx satisfies

uΞ΄βˆ’(x)βˆ’Ο†(x)≀uΞ΄βˆ’(x^)βˆ’Ο†(x^)forΒ everyΒ x∈V,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 y∈Vy\in V one has Θ(x^,y)=uΞ΄βˆ’(x^)βˆ’βŸ¨p,x^⟩Hβˆ’(vΞ΄+(y)βˆ’Οˆ(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 vΞ΄+(y)βˆ’Οˆ(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 Β§subsolution with Ξ΄\delta, the test function Ο†\varphi, the point x^\hat{x} and the number Ξ΅\varepsilon yields x1∈D(A)x_{1}\in D(A), s1∈Rs_{1}\in\mathbb{R}, p1∈Hp_{1}\in H and X1∈Sym(H)X_{1}\in\mathrm{Sym}(H) with

∣x1βˆ’x^∣H<Ξ΅,∣uΞ΄βˆ’(x1)βˆ’uΞ΄βˆ’(x^)∣<Ξ΅,∣s1βˆ’uΞ΄βˆ’(x^)∣<Ξ΅,∣p1βˆ’DΟ†(x^)∣H<Ξ΅,βˆ₯X1βˆ’Ξ±IHβˆ₯<Ξ΅,|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 FΞ΄βˆ’(x1,s1,p1,X1)≀ΡF^{-}_{\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 Β§supersolution with Ξ΄\delta, ψ\psi, y^\hat{y} and Ξ΅\varepsilon yields y1∈D(A)y_{1}\in D(A), t1∈Rt_{1}\in\mathbb{R}, q1∈Hq_{1}\in H and Y1∈Sym(H)Y_{1}\in\mathrm{Sym}(H) with

∣y1βˆ’y^∣H<Ξ΅,∣vΞ΄+(y1)βˆ’vΞ΄+(y^)∣<Ξ΅,∣t1βˆ’vΞ΄+(y^)∣<Ξ΅,∣q1βˆ’Dψ(y^)∣H<Ξ΅,βˆ₯Y1+Ξ±IHβˆ₯<Ξ΅,|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 βˆ’Ξ΅β‰€FΞ΄+(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 Ξ΄\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity Β§bound, uΞ΄βˆ’(x1)≀Cβˆ’Ξ΄h(x1)u^{-}_{\delta}(x_{1})\le C-\delta h(x_{1}), so, using C≀BC\le B, βˆ’uΞ΄βˆ’(x^)≀B-u^{-}_{\delta}(\hat{x})\le B and Ρ≀1\varepsilon\le1,

Ξ΄h(x1)≀Cβˆ’uΞ΄βˆ’(x1)≀Cβˆ’uΞ΄βˆ’(x^)+Ρ≀2B+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+1Ξ΄<Rh(x_{1})\le\frac{2B+1}{\delta}<R. By the same claim βˆ’C+Ξ΄h(y1)≀vΞ΄+(y1)-C+\delta h(y_{1})\le v^{+}_{\delta}(y_{1}), so Ξ΄h(y1)≀vΞ΄+(y1)+C≀vΞ΄+(y^)+Ξ΅+C≀2B+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 ∣s1βˆ£β‰€βˆ£uΞ΄βˆ’(x^)∣+Ρ≀B+1<R|s_{1}|\le|u^{-}_{\delta}(\hat{x})|+\varepsilon\le B+1<R and ∣t1βˆ£β‰€B+1<R|t_{1}|\le B+1<R, because B+1≀3B+2<RB+1\le3B+2<R and 0≀B0\le B.

Since ∣IH(x,y)∣=∣⟨x,y⟩Hβˆ£β‰€βˆ£x∣H∣y∣H|I_{H}(x,y)|=|\langle x,y\rangle_{H}|\le|x|_{H}|y|_{H} for x,y∈Hx,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 βˆ₯IHβˆ₯≀1\lVert I_{H}\rVert\le1, and hence βˆ₯Ξ±IHβˆ₯≀α\lVert\alpha I_{H}\rVert\le\alpha and βˆ₯βˆ’Ξ±IHβˆ₯≀α\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 Β§norm-axioms. Therefore, by the triangle inequality of that same claim,

βˆ₯X1βˆ₯≀βˆ₯Ξ±IHβˆ₯+βˆ₯X1βˆ’Ξ±IHβˆ₯≀α+1<R,βˆ₯Y1βˆ₯≀α+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 Β§triangle,

∣p1∣Hβ‰€βˆ£DΟ†(x^)∣H+Ξ΅β‰€Ξ±βˆ£x^βˆ’y^∣H+∣p∣H+Ρ≀G+Οƒ+Ρ≀G+2<G+2Ξ±<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<Ξ±1<\alpha, and likewise ∣q1∣H≀G+2<R|q_{1}|_{H}\le G+2<R. Thus ΞΎ1=(x1,s1,p1,X1)\xi_{1}=(x_{1},s_{1},p_{1},X_{1}) and Ξ·1=(y1,t1,q1,Y1)\eta_{1}=(y_{1},t_{1},q_{1},Y_{1}) are RR-bounded test data, and

FΞ΄βˆ’(ΞΎ1)βˆ’FΞ΄+(Ξ·1)≀Ρ+Ρ≀2<Ξ±+1<R.F^{-}_{\delta}(\xi_{1})-F^{+}_{\delta}(\eta_{1})\le\varepsilon+\varepsilon\le2<\alpha+1<R .

Hence ΞΎ1∈SΞ΄,Rβˆ’\xi_{1}\in S^{-}_{\delta,R} and Ξ·1∈SΞ΄,R+\eta_{1}\in S^{+}_{\delta,R} by Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets Β§admissible, each datum serving as the witness required for the other.

Step 4 (moving the gradient arguments). Put P=Ξ±(x1βˆ’y1)P=\alpha(x_{1}-y_{1}), Ο„1=∣Pβˆ’p1∣H\tau_{1}=|P-p_{1}|_{H} and Ο„2=∣Pβˆ’q1∣H\tau_{2}=|P-q_{1}|_{H}; these are nonnegative. By the triangle inequality,

Ο„1β‰€Ξ±βˆ£(x1βˆ’y1)βˆ’(x^βˆ’y^)∣H+∣α(x^βˆ’y^)+pβˆ’p1∣H+∣p∣H≀α(Ξ΅+Ξ΅)+Ξ΅+Οƒ=(2Ξ±+1)Ξ΅+Οƒ,\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 Ο„2\tau_{2}, since Dψ(y^)=Ξ±(x^βˆ’y^)βˆ’qD\psi(\hat{y})=\alpha(\hat{x}-\hat{y})-q and ∣q∣H≀σ|q|_{H}\le\sigma.

Apply the first condition of The Shift-Continuity Condition on Admissible Test Data Β§modulus to ΞΎ1\xi_{1} with the perturbations Pβˆ’p1∈HP-p_{1}\in H and 0Sym∈Sym(H)0_{\mathrm{Sym}}\in\mathrm{Sym}(H): since p1+(Pβˆ’p1)=Pp_{1}+(P-p_{1})=P, X1+0Sym=X1X_{1}+0_{\mathrm{Sym}}=X_{1} and βˆ₯0Symβˆ₯=0\lVert 0_{\mathrm{Sym}}\rVert=0,

FΞ΄βˆ’(x1,s1,P,X1)≀FΞ΄βˆ’(x1,s1,p1,X1)+Ο‰(Ο„1)≀Ρ+Ο‰(Ο„1).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 Ξ·1\eta_{1} with the perturbations Pβˆ’q1P-q_{1} and 0Sym0_{\mathrm{Sym}}:

βˆ’Ξ΅βˆ’Ο‰(Ο„2)≀FΞ΄+(y1,t1,q1,Y1)βˆ’Ο‰(Ο„2)≀FΞ΄+(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,y1∈D(A)=Wx_{1},y_{1}\in D(A)=W, ∣t1βˆ£β‰€B+1≀3B+2|t_{1}|\le B+1\le3B+2, 1<Ξ±1<\alpha, 0<Ξ΄<10<\delta<1 and P=Ξ±(x1βˆ’y1)P=\alpha(x_{1}-y_{1}), so The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple Β§pair, applied to the structure pair (Ο‰1,Ο‰2)(\omega_{1},\omega_{2}) at 3B+23B+2 with the value argument t1t_{1} and the form arguments X1X_{1} and Y1Y_{1}, gives

FΞ΄+(y1,t1,P,Y1)βˆ’Ο‰1(α∣x1βˆ’y1∣H2+1Ξ±)βˆ’Ο‰2(δ (h(x1)+h(y1)+1), α) ≀ FΞ΄βˆ’(x1,t1,P,X1).F^{+}_{\delta}(y_{1},t_{1},P,Y_{1})-\omega_{1}\Bigl(\alpha|x_{1}-y_{1}|_{H}^{2}+\tfrac{1}{\alpha}\Bigr)-\omega_{2}\bigl(\delta\,(h(x_{1})+h(y_{1})+1),\,\alpha\bigr)\ \le\ F^{-}_{\delta}(x_{1},t_{1},P,X_{1}).

Write Ξ©\Omega for the sum Ο‰1(α∣x1βˆ’y1∣H2+1Ξ±)+Ο‰2(δ (h(x1)+h(y1)+1), α)\omega_{1}\bigl(\alpha|x_{1}-y_{1}|_{H}^{2}+\tfrac{1}{\alpha}\bigr)+\omega_{2}\bigl(\delta\,(h(x_{1})+h(y_{1})+1),\,\alpha\bigr); it is nonnegative, because Ο‰1\omega_{1} and the function t↦ω2(t,Ξ±)t\mapsto\omega_{2}(t,\alpha) are moduli of continuity, whose values are nonnegative by clause 1 of Modulus of Continuity.

Step 6 (properness and conclusion). Since ∣s1βˆ’uΞ΄βˆ’(x^)∣<Ξ΅|s_{1}-u^{-}_{\delta}(\hat{x})|<\varepsilon and ∣t1βˆ’vΞ΄+(y^)∣<Ξ΅|t_{1}-v^{+}_{\delta}(\hat{y})|<\varepsilon,

uΞ΄βˆ’(x^)βˆ’vΞ΄+(y^)≀(s1+Ξ΅)βˆ’(t1βˆ’Ξ΅)=s1βˆ’t1+2Ξ΅.(βˆ—)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 t1≀s1t_{1}\le s_{1}. By Step 3 we have 0≀δh(x1)≀2B+10\le\delta h(x_{1})\le2B+1, ∣s1βˆ£β‰€B+1|s_{1}|\le B+1 and ∣t1βˆ£β‰€B+1|t_{1}|\le B+1, so both s1+Ξ΄h(x1)s_{1}+\delta h(x_{1}) and t1+Ξ΄h(x1)t_{1}+\delta h(x_{1}) lie between βˆ’(3B+2)-(3B+2) and 3B+23B+2, and t1+Ξ΄h(x1)≀s1+Ξ΄h(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 Β§constant at the level 3B+23B+2, with the point x1x_{1}, the gradient argument P+Ξ΄Ax1∈HP+\delta Ax_{1}\in H and the form argument X1∣V+Ξ΄IV∈Sym(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 Ξ΄\delta-Shifts Β§shifted, we obtain

Ξ»(s1βˆ’t1)=Ξ»((s1+Ξ΄h(x1))βˆ’(t1+Ξ΄h(x1)))≀FΞ΄βˆ’(x1,s1,P,X1)βˆ’FΞ΄βˆ’(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,

Ξ»(s1βˆ’t1)≀Ρ+Ο‰(Ο„1)βˆ’FΞ΄+(y1,t1,P,Y1)+Ω ≀ 2Ξ΅+Ο‰(Ο„1)+Ο‰(Ο„2)+Ξ©.\lambda(s_{1}-t_{1})\le\varepsilon+\omega(\tau_{1})-F^{+}_{\delta}(y_{1},t_{1},P,Y_{1})+\Omega\ \le\ 2\varepsilon+\omega(\tau_{1})+\omega(\tau_{2})+\Omega .

Multiplying (βˆ—)(*) by the positive number Ξ»\lambda and adding 2λΡ2\lambda\varepsilon to the previous display gives the asserted estimate.

Suppose now that s1<t1s_{1}<t_{1}. Then (βˆ—)(*) gives uΞ΄βˆ’(x^)βˆ’vΞ΄+(y^)<2Ξ΅u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})<2\varepsilon, so Ξ»(uΞ΄βˆ’(x^)βˆ’vΞ΄+(y^))<2λΡ\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 modulus of continuity Ο‰\omega are nonnegative by clause 1 of Modulus of Continuity, Ξ©\Omega is nonnegative by Step 5, and 0<2Ξ΅0<2\varepsilon.

In both cases x1,y1∈D(A)x_{1},y_{1}\in D(A) satisfy ∣x1βˆ’x^∣H<Ξ΅|x_{1}-\hat{x}|_{H}<\varepsilon, ∣y1βˆ’y^∣H<Ξ΅|y_{1}-\hat{y}|_{H}<\varepsilon, ∣uΞ΄βˆ’(x1)βˆ’uΞ΄βˆ’(x^)∣<Ξ΅|u^{-}_{\delta}(x_{1})-u^{-}_{\delta}(\hat{x})|<\varepsilon and ∣vΞ΄+(y1)βˆ’vΞ΄+(y^)∣<Ξ΅|v^{+}_{\delta}(y_{1})-v^{+}_{\delta}(\hat{y})|<\varepsilon by Step 2, and Ο„1,Ο„2\tau_{1},\tau_{2} satisfy the stated bounds by Step 4.

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