Each result cited is universally quantified over the data in its own statement. Write Ξ : V Γ V β R \Theta:V\times V\to\mathbb{R} Ξ : V Γ V β R for the function in the hypothesis, so that Ξ \Theta Ξ attains a maximum at ( x ^ , y ^ ) (\hat{x},\hat{y}) ( x ^ , y ^ β ) .
Step 1 (test functions). Let Ο : H β R \varphi:H\to\mathbb{R} Ο : H β R be given by Ο ( x ) = Ξ± 2 β£ x β y ^ β£ H 2 + β¨ p , x β© H \varphi(x)=\tfrac{\alpha}{2}|x-\hat{y}|_{H}^{2}+\langle p,x\rangle_{H} Ο ( x ) = 2 Ξ± β β£ x β y ^ β β£ H 2 β + β¨ p , x β© H β . By claims 3 and 1 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C 2 C^2 C 2 its two summands belong to C 2 ( H ) C^{2}(H) C 2 ( H ) , with gradients Ξ± ( x β y ^ ) \alpha(x-\hat{y}) Ξ± ( x β y ^ β ) and p p p and Hessians Ξ± I H \alpha I_{H} Ξ± I H β and 0 S y m 0_{\mathrm{Sym}} 0 Sym β at every x β H x\in H x β 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 β C 2 ( H ) \varphi\in C^{2}(H) Ο β C 2 ( H ) with
D Ο ( x ^ ) = Ξ± ( x ^ β y ^ ) + p , D 2 Ο ( x ^ ) = Ξ± I H . D\varphi(\hat{x})=\alpha(\hat{x}-\hat{y})+p,\qquad D^{2}\varphi(\hat{x})=\alpha I_{H}. D Ο ( x ^ ) = Ξ± ( x ^ β y ^ β ) + p , D 2 Ο ( x ^ ) = Ξ± I H β .
Let Ο : H β R \psi:H\to\mathbb{R} Ο : H β R be given by Ο ( y ) = β Ξ± 2 β£ y β x ^ β£ H 2 β β¨ q , y β© H \psi(y)=-\tfrac{\alpha}{2}|y-\hat{x}|_{H}^{2}-\langle q,y\rangle_{H} Ο ( y ) = β 2 Ξ± β β£ y β x ^ β£ H 2 β β β¨ q , y β© H β ; 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 , Ο β C 2 ( H ) \psi\in C^{2}(H) Ο β C 2 ( H ) with
D Ο ( y ^ ) = β Ξ± ( y ^ β x ^ ) β q = Ξ± ( x ^ β y ^ ) β q , D 2 Ο ( y ^ ) = β Ξ± I H . 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}. D Ο ( y ^ β ) = β Ξ± ( y ^ β β x ^ ) β q = Ξ± ( x ^ β y ^ β ) β q , D 2 Ο ( y ^ β ) = β Ξ± I H β .
For x β V x\in V x β V one has Ξ ( x , y ^ ) = ( u Ξ΄ β ( x ) β Ο ( x ) ) β v Ξ΄ + ( y ^ ) β β¨ q , y ^ β© H \Theta(x,\hat{y})=\bigl(u^{-}_{\delta}(x)-\varphi(x)\bigr)-v^{+}_{\delta}(\hat{y})-\langle q,\hat{y}\rangle_{H} Ξ ( x , y ^ β ) = ( u Ξ΄ β β ( x ) β Ο ( x ) ) β v Ξ΄ + β ( y ^ β ) β β¨ q , y ^ β β© H β , and Ξ ( x , y ^ ) β€ Ξ ( x ^ , y ^ ) \Theta(x,\hat{y})\le\Theta(\hat{x},\hat{y}) Ξ ( x , y ^ β ) β€ Ξ ( x ^ , y ^ β ) ; hence the function on V V V with value u Ξ΄ β ( x ) β Ο ( x ) u^{-}_{\delta}(x)-\varphi(x) u Ξ΄ β β ( x ) β Ο ( x ) at x x x satisfies
u Ξ΄ β ( x ) β Ο ( x ) β€ u Ξ΄ β ( x ^ ) β Ο ( x ^ ) forΒ everyΒ x β V , u^{-}_{\delta}(x)-\varphi(x)\le u^{-}_{\delta}(\hat{x})-\varphi(\hat{x})\qquad\text{for every }x\in V, u Ξ΄ β β ( x ) β Ο ( x ) β€ u Ξ΄ β β ( x ^ ) β Ο ( x ^ ) forΒ everyΒ x β V ,
and so has a local maximum relative to V V V at x ^ \hat{x} 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 β V y\in V y β V one has Ξ ( x ^ , y ) = u Ξ΄ β ( x ^ ) β β¨ p , x ^ β© H β ( v Ξ΄ + ( y ) β Ο ( y ) ) \Theta(\hat{x},y)=u^{-}_{\delta}(\hat{x})-\langle p,\hat{x}\rangle_{H}-\bigl(v^{+}_{\delta}(y)-\psi(y)\bigr) Ξ ( x ^ , y ) = u Ξ΄ β β ( x ^ ) β β¨ p , x ^ β© H β β ( v Ξ΄ + β ( y ) β Ο ( y ) ) , so the function with value v Ξ΄ + ( y ) β Ο ( y ) v^{+}_{\delta}(y)-\psi(y) v Ξ΄ + β ( y ) β Ο ( y ) at y y y has a local minimum relative to V V V at y ^ \hat{y} y ^ β .
Step 2 (test data). Applying Viscosity Subsolution, Supersolution and Solution of a Second-Order Equation on a Hilbert Triple Β§subsolution with Ξ΄ \delta Ξ΄ , the test function Ο \varphi Ο , the point x ^ \hat{x} x ^ and the number Ξ΅ \varepsilon Ξ΅ yields x 1 β D ( A ) x_{1}\in D(A) x 1 β β D ( A ) , s 1 β R s_{1}\in\mathbb{R} s 1 β β R , p 1 β H p_{1}\in H p 1 β β H and X 1 β S y m ( H ) X_{1}\in\mathrm{Sym}(H) X 1 β β Sym ( H ) with
β£ x 1 β x ^ β£ H < Ξ΅ , β£ u Ξ΄ β ( x 1 ) β u Ξ΄ β ( x ^ ) β£ < Ξ΅ , β£ s 1 β u Ξ΄ β ( x ^ ) β£ < Ξ΅ , β£ p 1 β D Ο ( x ^ ) β£ H < Ξ΅ , β₯ X 1 β Ξ± I H β₯ < 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, β£ x 1 β β x ^ β£ H β < Ξ΅ , β£ u Ξ΄ β β ( x 1 β ) β u Ξ΄ β β ( x ^ ) β£ < Ξ΅ , β£ s 1 β β u Ξ΄ β β ( x ^ ) β£ < Ξ΅ , β£ p 1 β β D Ο ( x ^ ) β£ H β < Ξ΅ , β₯ X 1 β β Ξ± I H β β₯ < Ξ΅ ,
and F Ξ΄ β ( x 1 , s 1 , p 1 , X 1 ) β€ Ξ΅ F^{-}_{\delta}(x_{1},s_{1},p_{1},X_{1})\le\varepsilon F Ξ΄ β β ( x 1 β , s 1 β , p 1 β , X 1 β ) β€ Ξ΅ . Applying Viscosity Subsolution, Supersolution and Solution of a Second-Order Equation on a Hilbert Triple Β§supersolution with Ξ΄ \delta Ξ΄ , Ο \psi Ο , y ^ \hat{y} y ^ β and Ξ΅ \varepsilon Ξ΅ yields y 1 β D ( A ) y_{1}\in D(A) y 1 β β D ( A ) , t 1 β R t_{1}\in\mathbb{R} t 1 β β R , q 1 β H q_{1}\in H q 1 β β H and Y 1 β S y m ( H ) Y_{1}\in\mathrm{Sym}(H) Y 1 β β Sym ( H ) with
β£ y 1 β y ^ β£ H < Ξ΅ , β£ v Ξ΄ + ( y 1 ) β v Ξ΄ + ( y ^ ) β£ < Ξ΅ , β£ t 1 β v Ξ΄ + ( y ^ ) β£ < Ξ΅ , β£ q 1 β D Ο ( y ^ ) β£ H < Ξ΅ , β₯ Y 1 + Ξ± I H β₯ < 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, β£ y 1 β β y ^ β β£ H β < Ξ΅ , β£ v Ξ΄ + β ( y 1 β ) β v Ξ΄ + β ( y ^ β ) β£ < Ξ΅ , β£ t 1 β β v Ξ΄ + β ( y ^ β ) β£ < Ξ΅ , β£ q 1 β β D Ο ( y ^ β ) β£ H β < Ξ΅ , β₯ Y 1 β + Ξ± I H β β₯ < Ξ΅ ,
and β Ξ΅ β€ F Ξ΄ + ( y 1 , t 1 , q 1 , Y 1 ) -\varepsilon\le F^{+}_{\delta}(y_{1},t_{1},q_{1},Y_{1}) β Ξ΅ β€ F Ξ΄ + β ( y 1 β , t 1 β , q 1 β , Y 1 β ) .
Step 3 (the data are admissible). By Basic Properties of the Ξ΄ \delta Ξ΄ -Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity Β§bound , u Ξ΄ β ( x 1 ) β€ C β Ξ΄ h ( x 1 ) u^{-}_{\delta}(x_{1})\le C-\delta h(x_{1}) u Ξ΄ β β ( x 1 β ) β€ C β Ξ΄ h ( x 1 β ) , so, using C β€ B C\le B C β€ B , β u Ξ΄ β ( x ^ ) β€ B -u^{-}_{\delta}(\hat{x})\le B β u Ξ΄ β β ( x ^ ) β€ B and Ξ΅ β€ 1 \varepsilon\le1 Ξ΅ β€ 1 ,
Ξ΄ h ( x 1 ) β€ C β u Ξ΄ β ( x 1 ) β€ C β u Ξ΄ β ( x ^ ) + Ξ΅ β€ 2 B + 1 , \delta h(x_{1})\le C-u^{-}_{\delta}(x_{1})\le C-u^{-}_{\delta}(\hat{x})+\varepsilon\le 2B+1 , Ξ΄ h ( x 1 β ) β€ C β u Ξ΄ β β ( x 1 β ) β€ C β u Ξ΄ β β ( x ^ ) + Ξ΅ β€ 2 B + 1 ,
whence h ( x 1 ) β€ 2 B + 1 Ξ΄ < R h(x_{1})\le\frac{2B+1}{\delta}<R h ( x 1 β ) β€ Ξ΄ 2 B + 1 β < R . By the same claim β C + Ξ΄ h ( y 1 ) β€ v Ξ΄ + ( y 1 ) -C+\delta h(y_{1})\le v^{+}_{\delta}(y_{1}) β C + Ξ΄ h ( y 1 β ) β€ v Ξ΄ + β ( y 1 β ) , so Ξ΄ h ( y 1 ) β€ v Ξ΄ + ( y 1 ) + C β€ v Ξ΄ + ( y ^ ) + Ξ΅ + C β€ 2 B + 1 \delta h(y_{1})\le v^{+}_{\delta}(y_{1})+C\le v^{+}_{\delta}(\hat{y})+\varepsilon+C\le2B+1 Ξ΄ h ( y 1 β ) β€ v Ξ΄ + β ( y 1 β ) + C β€ v Ξ΄ + β ( y ^ β ) + Ξ΅ + C β€ 2 B + 1 and h ( y 1 ) < R h(y_{1})<R h ( y 1 β ) < R . Next β£ s 1 β£ β€ β£ u Ξ΄ β ( x ^ ) β£ + Ξ΅ β€ B + 1 < R |s_{1}|\le|u^{-}_{\delta}(\hat{x})|+\varepsilon\le B+1<R β£ s 1 β β£ β€ β£ u Ξ΄ β β ( x ^ ) β£ + Ξ΅ β€ B + 1 < R and β£ t 1 β£ β€ B + 1 < R |t_{1}|\le B+1<R β£ t 1 β β£ β€ B + 1 < R , because B + 1 β€ 3 B + 2 < R B+1\le3B+2<R B + 1 β€ 3 B + 2 < R and 0 β€ B 0\le B 0 β€ B .
Since β£ I H ( x , y ) β£ = β£ β¨ x , y β© H β£ β€ β£ x β£ H β£ y β£ H |I_{H}(x,y)|=|\langle x,y\rangle_{H}|\le|x|_{H}|y|_{H} β£ I H β ( x , y ) β£ = β£ β¨ x , y β© H β β£ β€ β£ x β£ H β β£ y β£ H β for x , y β H x,y\in H x , y β 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 β₯ I H β₯ β€ 1 \lVert I_{H}\rVert\le1 β₯ I H β β₯ β€ 1 , and hence β₯ Ξ± I H β₯ β€ Ξ± \lVert\alpha I_{H}\rVert\le\alpha β₯ Ξ± I H β β₯ β€ Ξ± and β₯ β Ξ± I H β₯ β€ Ξ± \lVert-\alpha I_{H}\rVert\le\alpha β₯ β Ξ± I H β β₯ β€ Ξ± 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,
β₯ X 1 β₯ β€ β₯ Ξ± I H β₯ + β₯ X 1 β Ξ± I H β₯ β€ Ξ± + 1 < R , β₯ Y 1 β₯ β€ Ξ± + 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 . β₯ X 1 β β₯ β€ β₯ Ξ± I H β β₯ + β₯ X 1 β β Ξ± I H β β₯ β€ Ξ± + 1 < R , β₯ Y 1 β β₯ β€ Ξ± + 1 < R .
Finally, by The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity Β§triangle ,
β£ p 1 β£ H β€ β£ D Ο ( x ^ ) β£ H + Ξ΅ β€ Ξ± β£ x ^ β y ^ β£ H + β£ p β£ H + Ξ΅ β€ G + Ο + Ξ΅ β€ G + 2 < G + 2 Ξ± < 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, β£ p 1 β β£ H β β€ β£ D Ο ( x ^ ) β£ H β + Ξ΅ β€ Ξ± β£ x ^ β y ^ β β£ H β + β£ p β£ H β + Ξ΅ β€ G + Ο + Ξ΅ β€ G + 2 < G + 2 Ξ± < R ,
using 1 < Ξ± 1<\alpha 1 < Ξ± , and likewise β£ q 1 β£ H β€ G + 2 < R |q_{1}|_{H}\le G+2<R β£ q 1 β β£ H β β€ G + 2 < R . Thus ΞΎ 1 = ( x 1 , s 1 , p 1 , X 1 ) \xi_{1}=(x_{1},s_{1},p_{1},X_{1}) ΞΎ 1 β = ( x 1 β , s 1 β , p 1 β , X 1 β ) and Ξ· 1 = ( y 1 , t 1 , q 1 , Y 1 ) \eta_{1}=(y_{1},t_{1},q_{1},Y_{1}) Ξ· 1 β = ( y 1 β , t 1 β , q 1 β , Y 1 β ) are R R R -bounded test data, and
F Ξ΄ β ( ΞΎ 1 ) β F Ξ΄ + ( Ξ· 1 ) β€ Ξ΅ + Ξ΅ β€ 2 < Ξ± + 1 < R . F^{-}_{\delta}(\xi_{1})-F^{+}_{\delta}(\eta_{1})\le\varepsilon+\varepsilon\le2<\alpha+1<R . F Ξ΄ β β ( ΞΎ 1 β ) β F Ξ΄ + β ( Ξ· 1 β ) β€ Ξ΅ + Ξ΅ β€ 2 < Ξ± + 1 < R .
Hence ΞΎ 1 β S Ξ΄ , R β \xi_{1}\in S^{-}_{\delta,R} ΞΎ 1 β β S Ξ΄ , R β β and Ξ· 1 β S Ξ΄ , R + \eta_{1}\in S^{+}_{\delta,R} Ξ· 1 β β S Ξ΄ , R + β 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± ( x 1 β y 1 ) P=\alpha(x_{1}-y_{1}) P = Ξ± ( x 1 β β y 1 β ) , Ο 1 = β£ P β p 1 β£ H \tau_{1}=|P-p_{1}|_{H} Ο 1 β = β£ P β p 1 β β£ H β and Ο 2 = β£ P β q 1 β£ H \tau_{2}=|P-q_{1}|_{H} Ο 2 β = β£ P β q 1 β β£ H β ; these are nonnegative. By the triangle inequality,
Ο 1 β€ Ξ± β£ ( x 1 β y 1 ) β ( x ^ β y ^ ) β£ H + β£ Ξ± ( x ^ β y ^ ) + p β p 1 β£ H + β£ p β£ H β€ Ξ± ( Ξ΅ + Ξ΅ ) + Ξ΅ + Ο = ( 2 Ξ± + 1 ) Ξ΅ + Ο , \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 , Ο 1 β β€ Ξ± β ( x 1 β β y 1 β ) β ( x ^ β y ^ β ) β H β + β Ξ± ( x ^ β y ^ β ) + p β p 1 β β H β + β£ p β£ H β β€ Ξ± ( Ξ΅ + Ξ΅ ) + Ξ΅ + Ο = ( 2 Ξ± + 1 ) Ξ΅ + Ο ,
and the same bound holds for Ο 2 \tau_{2} Ο 2 β , since D Ο ( y ^ ) = Ξ± ( x ^ β y ^ ) β q D\psi(\hat{y})=\alpha(\hat{x}-\hat{y})-q D Ο ( y ^ β ) = Ξ± ( x ^ β y ^ β ) β q and β£ q β£ H β€ Ο |q|_{H}\le\sigma β£ q β£ H β β€ Ο .
Apply the first condition of The Shift-Continuity Condition on Admissible Test Data Β§modulus to ΞΎ 1 \xi_{1} ΞΎ 1 β with the perturbations P β p 1 β H P-p_{1}\in H P β p 1 β β H and 0 S y m β S y m ( H ) 0_{\mathrm{Sym}}\in\mathrm{Sym}(H) 0 Sym β β Sym ( H ) : since p 1 + ( P β p 1 ) = P p_{1}+(P-p_{1})=P p 1 β + ( P β p 1 β ) = P , X 1 + 0 S y m = X 1 X_{1}+0_{\mathrm{Sym}}=X_{1} X 1 β + 0 Sym β = X 1 β and β₯ 0 S y m β₯ = 0 \lVert 0_{\mathrm{Sym}}\rVert=0 β₯ 0 Sym β β₯ = 0 ,
F Ξ΄ β ( x 1 , s 1 , P , X 1 ) β€ F Ξ΄ β ( x 1 , s 1 , p 1 , X 1 ) + Ο ( Ο 1 ) β€ Ξ΅ + 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}). F Ξ΄ β β ( x 1 β , s 1 β , P , X 1 β ) β€ F Ξ΄ β β ( x 1 β , s 1 β , p 1 β , X 1 β ) + Ο ( Ο 1 β ) β€ Ξ΅ + Ο ( Ο 1 β ) .
Apply the second condition to Ξ· 1 \eta_{1} Ξ· 1 β with the perturbations P β q 1 P-q_{1} P β q 1 β and 0 S y m 0_{\mathrm{Sym}} 0 Sym β :
β Ξ΅ β Ο ( Ο 2 ) β€ F Ξ΄ + ( y 1 , t 1 , q 1 , Y 1 ) β Ο ( Ο 2 ) β€ F Ξ΄ + ( y 1 , t 1 , P , Y 1 ) . -\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}). β Ξ΅ β Ο ( Ο 2 β ) β€ F Ξ΄ + β ( y 1 β , t 1 β , q 1 β , Y 1 β ) β Ο ( Ο 2 β ) β€ F Ξ΄ + β ( y 1 β , t 1 β , P , Y 1 β ) .
Step 5 (the structure condition). We have x 1 , y 1 β D ( A ) = W x_{1},y_{1}\in D(A)=W x 1 β , y 1 β β D ( A ) = W , β£ t 1 β£ β€ B + 1 β€ 3 B + 2 |t_{1}|\le B+1\le3B+2 β£ t 1 β β£ β€ B + 1 β€ 3 B + 2 , 1 < Ξ± 1<\alpha 1 < Ξ± , 0 < Ξ΄ < 1 0<\delta<1 0 < Ξ΄ < 1 and P = Ξ± ( x 1 β y 1 ) P=\alpha(x_{1}-y_{1}) P = Ξ± ( x 1 β β y 1 β ) , 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}) ( Ο 1 β , Ο 2 β ) at 3 B + 2 3B+2 3 B + 2 with the value argument t 1 t_{1} t 1 β and the form arguments X 1 X_{1} X 1 β and Y 1 Y_{1} Y 1 β , gives
F Ξ΄ + ( y 1 , t 1 , P , Y 1 ) β Ο 1 ( Ξ± β£ x 1 β y 1 β£ H 2 + 1 Ξ± ) β Ο 2 ( Ξ΄ β ( h ( x 1 ) + h ( y 1 ) + 1 ) , β Ξ± ) Β β€ Β F Ξ΄ β ( x 1 , t 1 , P , X 1 ) . 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}). F Ξ΄ + β ( y 1 β , t 1 β , P , Y 1 β ) β Ο 1 β ( Ξ± β£ x 1 β β y 1 β β£ H 2 β + Ξ± 1 β ) β Ο 2 β ( Ξ΄ ( h ( x 1 β ) + h ( y 1 β ) + 1 ) , Ξ± ) Β β€ Β F Ξ΄ β β ( x 1 β , t 1 β , P , X 1 β ) .
Write Ξ© \Omega Ξ© for the sum Ο 1 ( Ξ± β£ x 1 β y 1 β£ H 2 + 1 Ξ± ) + Ο 2 ( Ξ΄ β ( h ( x 1 ) + h ( y 1 ) + 1 ) , β Ξ± ) \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) Ο 1 β ( Ξ± β£ x 1 β β y 1 β β£ H 2 β + Ξ± 1 β ) + Ο 2 β ( Ξ΄ ( h ( x 1 β ) + h ( y 1 β ) + 1 ) , Ξ± ) ; it is nonnegative, because Ο 1 \omega_{1} Ο 1 β and the function t β¦ Ο 2 ( t , Ξ± ) t\mapsto\omega_{2}(t,\alpha) t β¦ Ο 2 β ( t , Ξ± ) are moduli of continuity, whose values are nonnegative by clause 1 of Modulus of Continuity .
Step 6 (properness and conclusion). Since β£ s 1 β u Ξ΄ β ( x ^ ) β£ < Ξ΅ |s_{1}-u^{-}_{\delta}(\hat{x})|<\varepsilon β£ s 1 β β u Ξ΄ β β ( x ^ ) β£ < Ξ΅ and β£ t 1 β v Ξ΄ + ( y ^ ) β£ < Ξ΅ |t_{1}-v^{+}_{\delta}(\hat{y})|<\varepsilon β£ t 1 β β v Ξ΄ + β ( y ^ β ) β£ < Ξ΅ ,
u Ξ΄ β ( x ^ ) β v Ξ΄ + ( y ^ ) β€ ( s 1 + Ξ΅ ) β ( t 1 β Ξ΅ ) = s 1 β t 1 + 2 Ξ΅ . ( β ) u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\le(s_{1}+\varepsilon)-(t_{1}-\varepsilon)=s_{1}-t_{1}+2\varepsilon . \tag{$*$} u Ξ΄ β β ( x ^ ) β v Ξ΄ + β ( y ^ β ) β€ ( s 1 β + Ξ΅ ) β ( t 1 β β Ξ΅ ) = s 1 β β t 1 β + 2 Ξ΅ . ( β )
Suppose first that t 1 β€ s 1 t_{1}\le s_{1} t 1 β β€ s 1 β . By Step 3 we have 0 β€ Ξ΄ h ( x 1 ) β€ 2 B + 1 0\le\delta h(x_{1})\le2B+1 0 β€ Ξ΄ h ( x 1 β ) β€ 2 B + 1 , β£ s 1 β£ β€ B + 1 |s_{1}|\le B+1 β£ s 1 β β£ β€ B + 1 and β£ t 1 β£ β€ B + 1 |t_{1}|\le B+1 β£ t 1 β β£ β€ B + 1 , so both s 1 + Ξ΄ h ( x 1 ) s_{1}+\delta h(x_{1}) s 1 β + Ξ΄ h ( x 1 β ) and t 1 + Ξ΄ h ( x 1 ) t_{1}+\delta h(x_{1}) t 1 β + Ξ΄ h ( x 1 β ) lie between β ( 3 B + 2 ) -(3B+2) β ( 3 B + 2 ) and 3 B + 2 3B+2 3 B + 2 , and t 1 + Ξ΄ h ( x 1 ) β€ s 1 + Ξ΄ h ( x 1 ) t_{1}+\delta h(x_{1})\le s_{1}+\delta h(x_{1}) t 1 β + Ξ΄ h ( x 1 β ) β€ s 1 β + Ξ΄ h ( x 1 β ) . Applying Locally Strictly Proper Second-Order Equation Operator on a Hilbert Triple Β§constant at the level 3 B + 2 3B+2 3 B + 2 , with the point x 1 x_{1} x 1 β , the gradient argument P + Ξ΄ A x 1 β H P+\delta Ax_{1}\in H P + Ξ΄ A x 1 β β H and the form argument X 1 β£ V + Ξ΄ I V β S y m ( V ) X_{1}|_{V}+\delta I_{V}\in\mathrm{Sym}(V) X 1 β β£ V β + Ξ΄ I V β β Sym ( V ) , and reading the two resulting values of F F F through Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its Ξ΄ \delta Ξ΄ -Shifts Β§shifted , we obtain
Ξ» ( s 1 β t 1 ) = Ξ» ( ( s 1 + Ξ΄ h ( x 1 ) ) β ( t 1 + Ξ΄ h ( x 1 ) ) ) β€ F Ξ΄ β ( x 1 , s 1 , P , X 1 ) β F Ξ΄ β ( x 1 , t 1 , P , X 1 ) . \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}). Ξ» ( s 1 β β t 1 β ) = Ξ» ( ( s 1 β + Ξ΄ h ( x 1 β )) β ( t 1 β + Ξ΄ h ( x 1 β )) ) β€ F Ξ΄ β β ( x 1 β , s 1 β , P , X 1 β ) β F Ξ΄ β β ( x 1 β , t 1 β , P , X 1 β ) .
Combining this with Steps 4 and 5,
Ξ» ( s 1 β t 1 ) β€ Ξ΅ + Ο ( Ο 1 ) β F Ξ΄ + ( y 1 , t 1 , P , Y 1 ) + Ξ© Β β€ Β 2 Ξ΅ + 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 . Ξ» ( s 1 β β t 1 β ) β€ Ξ΅ + Ο ( Ο 1 β ) β F Ξ΄ + β ( y 1 β , t 1 β , P , Y 1 β ) + Ξ© Β β€ Β 2 Ξ΅ + Ο ( Ο 1 β ) + Ο ( Ο 2 β ) + Ξ©.
Multiplying ( β ) (*) ( β ) by the positive number Ξ» \lambda Ξ» and adding 2 Ξ» Ξ΅ 2\lambda\varepsilon 2 Ξ» Ξ΅ to the previous display gives the asserted estimate.
Suppose now that s 1 < t 1 s_{1}<t_{1} s 1 β < t 1 β . Then ( β ) (*) ( β ) gives u Ξ΄ β ( x ^ ) β v Ξ΄ + ( y ^ ) < 2 Ξ΅ u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})<2\varepsilon u Ξ΄ β β ( x ^ ) β v Ξ΄ + β ( y ^ β ) < 2 Ξ΅ , so Ξ» ( u Ξ΄ β ( x ^ ) β v Ξ΄ + ( y ^ ) ) < 2 Ξ» Ξ΅ \lambda\bigl(u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\bigr)<2\lambda\varepsilon Ξ» ( u Ξ΄ β β ( x ^ ) β v Ξ΄ + β ( y ^ β ) ) < 2 Ξ» Ξ΅ , and the asserted estimate holds because its remaining right-hand terms are nonnegative: the values of the modulus of continuity Ο \omega Ο are nonnegative by clause 1 of Modulus of Continuity , Ξ© \Omega Ξ© is nonnegative by Step 5, and 0 < 2 Ξ΅ 0<2\varepsilon 0 < 2 Ξ΅ .
In both cases x 1 , y 1 β D ( A ) x_{1},y_{1}\in D(A) x 1 β , y 1 β β D ( A ) satisfy β£ x 1 β x ^ β£ H < Ξ΅ |x_{1}-\hat{x}|_{H}<\varepsilon β£ x 1 β β x ^ β£ H β < Ξ΅ , β£ y 1 β y ^ β£ H < Ξ΅ |y_{1}-\hat{y}|_{H}<\varepsilon β£ y 1 β β y ^ β β£ H β < Ξ΅ , β£ u Ξ΄ β ( x 1 ) β u Ξ΄ β ( x ^ ) β£ < Ξ΅ |u^{-}_{\delta}(x_{1})-u^{-}_{\delta}(\hat{x})|<\varepsilon β£ u Ξ΄ β β ( x 1 β ) β u Ξ΄ β β ( x ^ ) β£ < Ξ΅ and β£ v Ξ΄ + ( y 1 ) β v Ξ΄ + ( y ^ ) β£ < Ξ΅ |v^{+}_{\delta}(y_{1})-v^{+}_{\delta}(\hat{y})|<\varepsilon β£ v Ξ΄ + β ( y 1 β ) β v Ξ΄ + β ( y ^ β ) β£ < Ξ΅ by Step 2, and Ο 1 , Ο 2 \tau_{1},\tau_{2} Ο 1 β , Ο 2 β satisfy the stated bounds by Step 4.