TheoremBase

The tail of the penalty is split off by an exact inequality that decouples the two variables and is sharp at the maximum point; the resulting functional is pushed to Euclidean space by fibre suprema, where the finite-dimensional lemma applies, and the Euclidean test data are lifted back by a perturbed maximum principle.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied here to the data named in the statement of the lemma.

Notation. Let Λ\Lambda, Λ♯\Lambda^{\sharp}, PP, the forms MΛM^{\Lambda} for M∈S(m)M\in\mathcal{S}(m), the projection form Π\Pi and the tail form NN be those determined by ee as in Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions, all of whose clauses are used throughout; in particular Λ\Lambda and Λ♯\Lambda^{\sharp} are linear, P=Λ♯ΛP=\Lambda^{\sharp}\Lambda, ∥Λx∥=∣Px∣≤∣x∣\lVert\Lambda x\rVert=|Px|\le|x|, ∣Λ♯ξ∣=∥ξ∥|\Lambda^{\sharp}\xi|=\lVert\xi\rVert, ∣x∣2=Π(x,x)+N(x,x)|x|^{2}=\Pi(x,x)+N(x,x) and N(x,x)=∣x−Px∣2N(x,x)=|x-Px|^{2}, so that ∣x−Px∣≤∣x∣|x-Px|\le|x|. Since ∣e1∣=1|e_{1}|=1 we have H≠{0H}H\ne\{0_{H}\}, so ∥I∥=1\lVert I\rVert=1 by claim 3 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity. Write

M0=Φ(xˉ,yˉ),zˉ=(xˉ−yˉ)−P(xˉ−yˉ),M_{0}=\Phi(\bar{x},\bar{y}),\qquad \bar{z}=(\bar{x}-\bar{y})-P(\bar{x}-\bar{y}),

and let g,k:H→Rg,k:H\to\mathbb{R} be given by

g(x)=−α ⟨zˉ,x−xˉ⟩−α N(x−xˉ,x−xˉ),k(y)=α ⟨zˉ,y−yˉ⟩−α N(y−yˉ,y−yˉ).g(x)=-\alpha\,\langle\bar{z},x-\bar{x}\rangle-\alpha\,N(x-\bar{x},x-\bar{x}), \qquad k(y)=\alpha\,\langle\bar{z},y-\bar{y}\rangle-\alpha\,N(y-\bar{y},y-\bar{y}).

By clause 1 of Sequentially Strict Maxima and Minima on a Subset of a Metric Space (i), Φ(x,y)≤M0\Phi(x,y)\le M_{0} for all (x,y)∈A×A(x,y)\in A\times A. Every component of ee lies in AA, so AA is nonempty.

Claim 1 (splitting off the tail of the penalty). For all x,y∈Hx,y\in H,

−α2 N(x−y,x−y) ≥ −α2 ∣zˉ∣2+g(x)+k(y),-\tfrac{\alpha}{2}\,N(x-y,x-y)\ \ge\ -\tfrac{\alpha}{2}\,|\bar{z}|^{2}+g(x)+k(y),

with equality when x=xˉx=\bar{x} and y=yˉy=\bar{y}; moreover g(x)≤α4∣zˉ∣2g(x)\le\tfrac{\alpha}{4}|\bar{z}|^{2} and k(y)≤α4∣zˉ∣2k(y)\le\tfrac{\alpha}{4}|\bar{z}|^{2} for all x,y∈Hx,y\in H.

Proof. Put a=(x−xˉ)−P(x−xˉ)a=(x-\bar{x})-P(x-\bar{x}) and b=(y−yˉ)−P(y−yˉ)b=(y-\bar{y})-P(y-\bar{y}). Since PP is linear,

(x−y)−P(x−y)=a−b+zˉ,(x-y)-P(x-y)=a-b+\bar{z},

because (x−y)=(x−xˉ)−(y−yˉ)+(xˉ−yˉ)(x-y)=(x-\bar{x})-(y-\bar{y})+(\bar{x}-\bar{y}). By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iii),

N(x−y,x−y)=∣a−b+zˉ∣2,N(x−xˉ,x−xˉ)=∣a∣2,N(y−yˉ,y−yˉ)=∣b∣2,N(x-y,x-y)=|a-b+\bar{z}|^{2},\qquad N(x-\bar{x},x-\bar{x})=|a|^{2},\qquad N(y-\bar{y},y-\bar{y})=|b|^{2},

and, using the second expression N(z,w)=⟨z−Pz,w⟩N(z,w)=\langle z-Pz,w\rangle there together with the first,

⟨zˉ,x−xˉ⟩=N(xˉ−yˉ,x−xˉ)=⟨zˉ,a⟩,⟨zˉ,y−yˉ⟩=⟨zˉ,b⟩.\langle\bar{z},x-\bar{x}\rangle=N(\bar{x}-\bar{y},x-\bar{x})=\langle\bar{z},a\rangle, \qquad \langle\bar{z},y-\bar{y}\rangle=\langle\bar{z},b\rangle .

By Elementary Identities in a Real Inner Product Space (v) applied twice, and by Elementary Identities in a Real Inner Product Space (i),

∣a−b+zˉ∣2=∣a−b∣2+2⟨a−b,zˉ⟩+∣zˉ∣2=∣a−b∣2+2⟨zˉ,a⟩−2⟨zˉ,b⟩+∣zˉ∣2,|a-b+\bar{z}|^{2}=|a-b|^{2}+2\langle a-b,\bar{z}\rangle+|\bar{z}|^{2} =|a-b|^{2}+2\langle\bar{z},a\rangle-2\langle\bar{z},b\rangle+|\bar{z}|^{2},

and ∣a−b∣2=∣a∣2−2⟨a,b⟩+∣b∣2|a-b|^{2}=|a|^{2}-2\langle a,b\rangle+|b|^{2} while 0≤∣a+b∣2=∣a∣2+2⟨a,b⟩+∣b∣20\le|a+b|^{2}=|a|^{2}+2\langle a,b\rangle+|b|^{2}, so −2⟨a,b⟩≤∣a∣2+∣b∣2-2\langle a,b\rangle\le|a|^{2}+|b|^{2} and therefore ∣a−b∣2≤2∣a∣2+2∣b∣2|a-b|^{2}\le2|a|^{2}+2|b|^{2}. Hence

N(x−y,x−y)≤∣zˉ∣2+2⟨zˉ,a⟩−2⟨zˉ,b⟩+2∣a∣2+2∣b∣2.N(x-y,x-y)\le|\bar{z}|^{2}+2\langle\bar{z},a\rangle-2\langle\bar{z},b\rangle+2|a|^{2}+2|b|^{2}.

Multiplying by the positive number α2\tfrac{\alpha}{2} (claim 5 of Elementary Arithmetic in an Ordered Field) and reversing the sign (claim 4 of Elementary Order Arithmetic in an Ordered Field) gives

−α2N(x−y,x−y) ≥ −α2∣zˉ∣2−α⟨zˉ,a⟩+α⟨zˉ,b⟩−α∣a∣2−α∣b∣2=−α2∣zˉ∣2+g(x)+k(y),-\tfrac{\alpha}{2}N(x-y,x-y)\ \ge\ -\tfrac{\alpha}{2}|\bar{z}|^{2}-\alpha\langle\bar{z},a\rangle+\alpha\langle\bar{z},b\rangle-\alpha|a|^{2}-\alpha|b|^{2} =-\tfrac{\alpha}{2}|\bar{z}|^{2}+g(x)+k(y),

by the identities displayed above. If x=xˉx=\bar{x} and y=yˉy=\bar{y} then a=b=0Ha=b=0_{H}, so g(xˉ)=0g(\bar{x})=0, k(yˉ)=0k(\bar{y})=0 and N(xˉ−yˉ,xˉ−yˉ)=∣zˉ∣2N(\bar{x}-\bar{y},\bar{x}-\bar{y})=|\bar{z}|^{2}, and both sides equal −α2∣zˉ∣2-\tfrac{\alpha}{2}|\bar{z}|^{2}.

For the upper bounds, The Cauchy–Schwarz Inequality in a Real Inner Product Space and claims 1 and 3 of Properties of the Absolute Value in an Ordered Field give −⟨zˉ,a⟩≤∣⟨zˉ,a⟩∣≤∣zˉ∣ ∣a∣-\langle\bar{z},a\rangle\le|\langle\bar{z},a\rangle|\le|\bar{z}|\,|a|, so g(x)≤α∣zˉ∣∣a∣−α∣a∣2g(x)\le\alpha|\bar{z}||a|-\alpha|a|^{2} by claim 5 of Elementary Arithmetic in an Ordered Field. Since 0≤α(∣a∣−∣zˉ∣2)2=α∣a∣2−α∣zˉ∣∣a∣+α4∣zˉ∣20\le\alpha\bigl(|a|-\tfrac{|\bar{z}|}{2}\bigr)^{2}=\alpha|a|^{2}-\alpha|\bar{z}||a|+\tfrac{\alpha}{4}|\bar{z}|^{2}, we get α∣zˉ∣∣a∣−α∣a∣2≤α4∣zˉ∣2\alpha|\bar{z}||a|-\alpha|a|^{2}\le\tfrac{\alpha}{4}|\bar{z}|^{2}, whence g(x)≤α4∣zˉ∣2g(x)\le\tfrac{\alpha}{4}|\bar{z}|^{2}. The same computation with bb in place of aa bounds kk. This proves Claim 1.

Claim 2 (the decoupled functional). Let u^,v^:A→R\hat{u},\hat{v}:A\to\mathbb{R} be given by u^(x)=u(x)+g(x)\hat{u}(x)=u(x)+g(x) and v^(y)=v(y)−k(y)\hat{v}(y)=v(y)-k(y). Then the set of values of u^\hat{u} is bounded above and that of v^\hat{v} is bounded below;

u^(x)−v^(y)−α2∥Λx−Λy∥2−α2∣zˉ∣2 ≤ Φ(x,y)for all x,y∈A,\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2}-\tfrac{\alpha}{2}|\bar{z}|^{2}\ \le\ \Phi(x,y)\qquad\text{for all }x,y\in A,

with equality when x=xˉx=\bar{x}, y=yˉy=\bar{y}; and

u^(x)−v^(y)−α2∥Λx−Λy∥2 ≤ u^(xˉ)−v^(yˉ)−α2∥Λxˉ−Λyˉ∥2for all x,y∈A.\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2}\ \le\ \hat{u}(\bar{x})-\hat{v}(\bar{y})-\tfrac{\alpha}{2}\lVert\Lambda\bar{x}-\Lambda\bar{y}\rVert^{2}\qquad\text{for all }x,y\in A .

Proof. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (i) and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iii), ∥Λx−Λy∥=∥Λ(x−y)∥\lVert\Lambda x-\Lambda y\rVert=\lVert\Lambda(x-y)\rVert and ∣x−y∣2=∥Λ(x−y)∥2+N(x−y,x−y)|x-y|^{2}=\lVert\Lambda(x-y)\rVert^{2}+N(x-y,x-y). Hence, by Claim 1,

Φ(x,y)=u(x)−v(y)−α2∥Λx−Λy∥2−α2N(x−y,x−y) ≥ u(x)+g(x)−(v(y)−k(y))−α2∥Λx−Λy∥2−α2∣zˉ∣2,\Phi(x,y)=u(x)-v(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2}-\tfrac{\alpha}{2}N(x-y,x-y) \ \ge\ u(x)+g(x)-\bigl(v(y)-k(y)\bigr)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2}-\tfrac{\alpha}{2}|\bar{z}|^{2},

which is the first display; equality at (xˉ,yˉ)(\bar{x},\bar{y}) follows from the equality case of Claim 1. For the second display, the first one and Φ(x,y)≤M0\Phi(x,y)\le M_{0} give

u^(x)−v^(y)−α2∥Λx−Λy∥2≤Φ(x,y)+α2∣zˉ∣2≤M0+α2∣zˉ∣2,\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2}\le\Phi(x,y)+\tfrac{\alpha}{2}|\bar{z}|^{2}\le M_{0}+\tfrac{\alpha}{2}|\bar{z}|^{2},

and by the equality case the right-hand side equals u^(xˉ)−v^(yˉ)−α2∥Λxˉ−Λyˉ∥2\hat{u}(\bar{x})-\hat{v}(\bar{y})-\tfrac{\alpha}{2}\lVert\Lambda\bar{x}-\Lambda\bar{y}\rVert^{2}. Finally, let CuC_{u} be an upper bound for the values of uu and CvC_{v} one for the values of −v-v; by Claim 1, u^(x)≤Cu+α4∣zˉ∣2\hat{u}(x)\le C_{u}+\tfrac{\alpha}{4}|\bar{z}|^{2} and −v^(y)=−v(y)+k(y)≤Cv+α4∣zˉ∣2-\hat{v}(y)=-v(y)+k(y)\le C_{v}+\tfrac{\alpha}{4}|\bar{z}|^{2}, so the values of v^\hat{v} are bounded below. This proves Claim 2.

Claim 3 (the two forms, and clauses 2 to 5). Claim 2 supplies the hypotheses of Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes for the data AA, ee, u^\hat{u}, v^\hat{v}, α\alpha, xˉ\bar{x}, yˉ\bar{y}. Let UU, V\mathcal{V}, U∗U^{*}, V∗\mathcal{V}_{*}, ζˉ=Λxˉ\bar{\zeta}=\Lambda\bar{x} and ωˉ=Λyˉ\bar{\omega}=\Lambda\bar{y} be as there. By Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes (ii), U∗U^{*} is upper semicontinuous on Rm\mathbb{R}^{m}, V∗\mathcal{V}_{*} is lower semicontinuous on Rm\mathbb{R}^{m}, and

U∗(ζ)−V∗(ω)−α2∥ζ−ω∥2 ≤ U∗(ζˉ)−V∗(ωˉ)−α2∥ζˉ−ωˉ∥2for all ζ,ω∈Rm;U^{*}(\zeta)-\mathcal{V}_{*}(\omega)-\tfrac{\alpha}{2}\lVert\zeta-\omega\rVert^{2}\ \le\ U^{*}(\bar{\zeta})-\mathcal{V}_{*}(\bar{\omega})-\tfrac{\alpha}{2}\lVert\bar{\zeta}-\bar{\omega}\rVert^{2} \qquad\text{for all }\zeta,\omega\in\mathbb{R}^{m};

and by Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes (iii), U∗(ζˉ)=u^(xˉ)U^{*}(\bar{\zeta})=\hat{u}(\bar{x}) and V∗(ωˉ)=v^(yˉ)\mathcal{V}_{*}(\bar{\omega})=\hat{v}(\bar{y}).

The set Rm\mathbb{R}^{m} is open in Rm\mathbb{R}^{m} by claim 1 of Euclidean Space Is Open in Itself, so Ishii's Lemma: Test Data and Matrix Bounds at a Maximum of a Quadratically Penalised Difference applies with mm in the role of nn, with Ω=Rm\Omega=\mathbb{R}^{m}, with U∗U^{*} and V∗\mathcal{V}_{*} in the roles of uu and vv, with α\alpha, and with ζˉ\bar{\zeta} and ωˉ\bar{\omega} in the roles of the two points; its local hypothesis holds with δ=1\delta=1 because the displayed inequality holds for all ζ,ω\zeta,\omega. Writing p0=α(ζˉ−ωˉ)p_{0}=\alpha(\bar{\zeta}-\bar{\omega}), we obtain X0,Y0∈S(m)X_{0},Y_{0}\in\mathcal{S}(m) such that (i) the quadruple (ζˉ,U∗(ζˉ),p0,X0)(\bar{\zeta},U^{*}(\bar{\zeta}),p_{0},X_{0}) is approximable by test data from above for U∗U^{*} and (ωˉ,V∗(ωˉ),p0,Y0)(\bar{\omega},\mathcal{V}_{*}(\bar{\omega}),p_{0},Y_{0}) is approximable by test data from below for V∗\mathcal{V}_{*}, the open set being Rm\mathbb{R}^{m} in both cases (clause 1 there); (ii) for all ξ,η∈Rm\xi,\eta\in\mathbb{R}^{m},

−3α(∥ξ∥2+∥η∥2)≤ξ⋅(X0ξ)−η⋅(Y0η)≤3α∥ξ−η∥2-3\alpha\bigl(\lVert\xi\rVert^{2}+\lVert\eta\rVert^{2}\bigr)\le\xi\cdot(X_{0}\xi)-\eta\cdot(Y_{0}\eta)\le3\alpha\lVert\xi-\eta\rVert^{2}

(clause 3 there); (iii) X0⪯Y0X_{0}\preceq Y_{0} (clause 4 there); and (iv) ∥X0∥≤6α\lVert X_{0}\rVert\le6\alpha and ∥Y0∥≤6α\lVert Y_{0}\rVert\le6\alpha (clause 5 there).

Put X=X0ΛX=X_{0}^{\Lambda} and Y=Y0ΛY=Y_{0}^{\Lambda}, elements of Sym(H)\mathrm{Sym}(H) by Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (ii). Clause 5 is then the identity MΛ(z,w)=MΛ(Pz,Pw)M^{\Lambda}(z,w)=M^{\Lambda}(Pz,Pw) of that clause, clause 4 follows from (iv) and the bound ∥MΛ∥≤∥M∥\lVert M^{\Lambda}\rVert\le\lVert M\rVert there, and clause 3 follows from (iii) and the order transfer there. For clause 2, apply (ii) with ξ=Λz\xi=\Lambda z and η=Λw\eta=\Lambda w, so that ξ⋅(X0ξ)=X(z,z)\xi\cdot(X_{0}\xi)=X(z,z) and η⋅(Y0η)=Y(w,w)\eta\cdot(Y_{0}\eta)=Y(w,w). Since 0≤∥Λ(z−w)∥≤∣z−w∣0\le\lVert\Lambda(z-w)\rVert\le|z-w|, two applications of claim 5 of Elementary Arithmetic in an Ordered Field give ∥Λz−Λw∥2=∥Λ(z−w)∥2≤∣z−w∣2\lVert\Lambda z-\Lambda w\rVert^{2}=\lVert\Lambda(z-w)\rVert^{2}\le|z-w|^{2}, and multiplying by the nonnegative 3α3\alpha gives the upper bound of clause 2. Likewise ∥Λz∥2+∥Λw∥2≤∣z∣2+∣w∣2\lVert\Lambda z\rVert^{2}+\lVert\Lambda w\rVert^{2}\le|z|^{2}+|w|^{2}, so multiplying by 3α3\alpha and reversing the sign gives −3α(∣z∣2+∣w∣2)≤−3α(∥Λz∥2+∥Λw∥2)-3\alpha(|z|^{2}+|w|^{2})\le-3\alpha(\lVert\Lambda z\rVert^{2}+\lVert\Lambda w\rVert^{2}), which with (ii) gives the lower bound.

We record for later use that ζˉ−ωˉ=Λ(xˉ−yˉ)\bar{\zeta}-\bar{\omega}=\Lambda(\bar{x}-\bar{y}), so that by the linearity of Λ♯\Lambda^{\sharp} and P=Λ♯ΛP=\Lambda^{\sharp}\Lambda,

Λ♯p0=α P(xˉ−yˉ),whencep=α(xˉ−yˉ)=αP(xˉ−yˉ)+αzˉ=Λ♯p0+αzˉ.\Lambda^{\sharp}p_{0}=\alpha\,P(\bar{x}-\bar{y}), \qquad\text{whence}\qquad p=\alpha(\bar{x}-\bar{y})=\alpha P(\bar{x}-\bar{y})+\alpha\bar{z}=\Lambda^{\sharp}p_{0}+\alpha\bar{z}.

This proves Claim 3.

Claim 4 (clause 1). Let ε∈R\varepsilon\in\mathbb{R} be positive. We produce x1,y1∈Ax_{1},y_{1}\in A and φ,ψ∈C2(H)\varphi,\psi\in C^{2}(H) such that the function on AA with value u(x)−φ(x)u(x)-\varphi(x) at xx has a local maximum at x1x_{1} relative to AA, the function on AA with value v(y)−ψ(y)v(y)-\psi(y) at yy has a local minimum at y1y_{1} relative to AA, and

∣x1−xˉ∣<ε,∣u(x1)−u(xˉ)∣<ε,∣Dφ(x1)−p∣<ε,∥D2φ(x1)−(X+2αN)∥<ε,|x_{1}-\bar{x}|<\varepsilon,\quad |u(x_{1})-u(\bar{x})|<\varepsilon,\quad \bigl|D\varphi(x_{1})-p\bigr|<\varepsilon,\quad \bigl\lVert D^{2}\varphi(x_{1})-(X+2\alpha N)\bigr\rVert<\varepsilon, ∣y1−yˉ∣<ε,∣v(y1)−v(yˉ)∣<ε,∣Dψ(y1)−p∣<ε,∥D2ψ(y1)−(Y−2αN)∥<ε.|y_{1}-\bar{y}|<\varepsilon,\quad |v(y_{1})-v(\bar{y})|<\varepsilon,\quad \bigl|D\psi(y_{1})-p\bigr|<\varepsilon,\quad \bigl\lVert D^{2}\psi(y_{1})-(Y-2\alpha N)\bigr\rVert<\varepsilon .

Since ε\varepsilon is arbitrary, this is clause 1, by Quadruple Approximable by Test Data on a Subset of a Real Inner Product Space (i) and Quadruple Approximable by Test Data on a Subset of a Real Inner Product Space (ii).

Step 1 (the localisation radius). Let ε1\varepsilon_{1} be the lesser of ε\varepsilon and ε8α\tfrac{\varepsilon}{8\alpha}, positive because it is one of them. The function uu and the function −v-v have closed superlevel sets in HH, AA is nonempty, and Φ\Phi attains a sequentially strict maximum on A×AA\times A at (xˉ,yˉ)(\bar{x},\bar{y}), so Localisation at a Sequentially Strict Maximum of a Quadratically Penalised Difference (i) provides a positive η0∈R\eta_{0}\in\mathbb{R} such that every (x,y)∈A×A(x,y)\in A\times A with M0−η0<Φ(x,y)M_{0}-\eta_{0}<\Phi(x,y) satisfies

∣x−xˉ∣<ε1,∣y−yˉ∣<ε1,∣u(x)−u(xˉ)∣<ε1,∣v(y)−v(yˉ)∣<ε1.|x-\bar{x}|<\varepsilon_{1},\quad |y-\bar{y}|<\varepsilon_{1},\quad |u(x)-u(\bar{x})|<\varepsilon_{1},\quad |v(y)-v(\bar{y})|<\varepsilon_{1}.

Step 2 (accuracy of the Euclidean data). Put D0=∥ζˉ−ωˉ∥D_{0}=\lVert\bar{\zeta}-\bar{\omega}\rVert. Let ε′\varepsilon' be a positive real number with

ε′≤1,ε′≤ε16,ε′≤η016,2∣α∣ ε′ (D0+2)≤η016,\varepsilon'\le1,\qquad \varepsilon'\le\tfrac{\varepsilon}{16},\qquad \varepsilon'\le\tfrac{\eta_{0}}{16},\qquad 2|\alpha|\,\varepsilon'\,(D_{0}+2)\le\tfrac{\eta_{0}}{16},

which exists: the first three are satisfied by the least of 11, ε16\tfrac{\varepsilon}{16} and η016\tfrac{\eta_{0}}{16}, and the fourth by any positive number at most η016 (2∣α∣(D0+2)+1)\tfrac{\eta_{0}}{16\,(2|\alpha|(D_{0}+2)+1)}, so the least of these four positive numbers serves. Let η1\eta_{1} be a positive real with 2η1≤ε162\eta_{1}\le\tfrac{\varepsilon}{16}.

Step 3 (the Euclidean test data). By (i) of Claim 3 and Quadruple Approximable by Test-Function Data (i), applied with the accuracy ε′\varepsilon', there are ζ1∈Rm\zeta_{1}\in\mathbb{R}^{m} and a function χ:Rm→R\chi:\mathbb{R}^{m}\to\mathbb{R} of class C2C^{2} on Rm\mathbb{R}^{m} such that the function with value U∗(ζ)−χ(ζ)U^{*}(\zeta)-\chi(\zeta) at ζ\zeta has a local maximum at ζ1\zeta_{1} relative to Rm\mathbb{R}^{m} and

dE(ζ1,ζˉ)<ε′,∣U∗(ζ1)−U∗(ζˉ)∣<ε′,∥Dχ(ζ1)−p0∥<ε′,dS(m)(D2χ(ζ1),X0)<ε′.d_{E}(\zeta_{1},\bar{\zeta})<\varepsilon',\quad |U^{*}(\zeta_{1})-U^{*}(\bar{\zeta})|<\varepsilon',\quad \lVert D\chi(\zeta_{1})-p_{0}\rVert<\varepsilon',\quad d_{\mathcal{S}(m)}\bigl(D^{2}\chi(\zeta_{1}),X_{0}\bigr)<\varepsilon' .

Likewise, by Quadruple Approximable by Test-Function Data (ii), there are ω1∈Rm\omega_{1}\in\mathbb{R}^{m} and θ:Rm→R\theta:\mathbb{R}^{m}\to\mathbb{R} of class C2C^{2} on Rm\mathbb{R}^{m} such that the function with value V∗(ω)−θ(ω)\mathcal{V}_{*}(\omega)-\theta(\omega) at ω\omega has a local minimum at ω1\omega_{1} relative to Rm\mathbb{R}^{m} and the four analogous inequalities hold with ω1,θ,V∗,ωˉ,Y0\omega_{1},\theta,\mathcal{V}_{*},\bar{\omega},Y_{0} in place of ζ1,χ,U∗,ζˉ,X0\zeta_{1},\chi,U^{*},\bar{\zeta},X_{0}.

Step 4 (replacing the test functions by coordinate quadratics). Apply Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (v) with Ω=Rm\Omega=\mathbb{R}^{m}, with χ\chi, ζ1\zeta_{1} and the positive η1\eta_{1}: the associated quadratic

T0(ζ)=χ(ζ1)+Dχ(ζ1)⋅(ζ−ζ1)+12(ζ−ζ1)⋅(D2χ(ζ1)(ζ−ζ1))+η1∥ζ−ζ1∥2T_{0}(\zeta)=\chi(\zeta_{1})+D\chi(\zeta_{1})\cdot(\zeta-\zeta_{1})+\tfrac{1}{2}(\zeta-\zeta_{1})\cdot\bigl(D^{2}\chi(\zeta_{1})(\zeta-\zeta_{1})\bigr)+\eta_{1}\lVert\zeta-\zeta_{1}\rVert^{2}

satisfies T0(ζ1)=χ(ζ1)T_{0}(\zeta_{1})=\chi(\zeta_{1}), and there is a positive ρ1\rho_{1} with χ(ζ)≤T0(ζ)\chi(\zeta)\le T_{0}(\zeta) whenever ∥ζ−ζ1∥<ρ1\lVert\zeta-\zeta_{1}\rVert<\rho_{1}. Let ρ0\rho_{0} be positive and such that U∗(ζ)−χ(ζ)≤U∗(ζ1)−χ(ζ1)U^{*}(\zeta)-\chi(\zeta)\le U^{*}(\zeta_{1})-\chi(\zeta_{1}) for every ζ\zeta with dE(ζ,ζ1)<ρ0d_{E}(\zeta,\zeta_{1})<\rho_{0}, as the local maximum property provides. Then for every ζ\zeta with ∥ζ−ζ1∥\lVert\zeta-\zeta_{1}\rVert less than both ρ0\rho_{0} and ρ1\rho_{1},

U∗(ζ)−T0(ζ) ≤ U∗(ζ)−χ(ζ) ≤ U∗(ζ1)−χ(ζ1)=U∗(ζ1)−T0(ζ1).U^{*}(\zeta)-T_{0}(\zeta)\ \le\ U^{*}(\zeta)-\chi(\zeta)\ \le\ U^{*}(\zeta_{1})-\chi(\zeta_{1})=U^{*}(\zeta_{1})-T_{0}(\zeta_{1}).

Let T=T0∘ΛT=T_{0}\circ\Lambda. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iv), T∈C2(H)T\in C^{2}(H), T(x)T(x) depends only on Λx\Lambda x, the Hessian D2T(x)D^{2}T(x) equals the constant form

bu=(D2χ(ζ1))Λ+2η1 Π,b_{u}=\bigl(D^{2}\chi(\zeta_{1})\bigr)^{\Lambda}+2\eta_{1}\,\Pi ,

and ∣DT(x)−Λ♯Dχ(ζ1)∣≤(∥D2χ(ζ1)∥+2η1)∥Λx−ζ1∥\bigl|DT(x)-\Lambda^{\sharp}D\chi(\zeta_{1})\bigr|\le\bigl(\lVert D^{2}\chi(\zeta_{1})\rVert+2\eta_{1}\bigr)\lVert\Lambda x-\zeta_{1}\rVert for every x∈Hx\in H. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (ii) and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iii), together with claims 1 and 3 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity,

∥bu−X∥≤∥(D2χ(ζ1)−X0)Λ∥+2η1∥Π∥≤ε′+2η1.\lVert b_{u}-X\rVert\le\bigl\lVert\bigl(D^{2}\chi(\zeta_{1})-X_{0}\bigr)^{\Lambda}\bigr\rVert+2\eta_{1}\lVert\Pi\rVert\le\varepsilon'+2\eta_{1}.

Applying Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (v) instead with θ\theta, ω1\omega_{1} and the negative number −η1-\eta_{1} gives a quadratic S0S_{0} with S0(ω1)=θ(ω1)S_{0}(\omega_{1})=\theta(\omega_{1}) and a positive ρ1′\rho_{1}' with S0(ω)≤θ(ω)S_{0}(\omega)\le\theta(\omega) for ∥ω−ω1∥<ρ1′\lVert\omega-\omega_{1}\rVert<\rho_{1}'; with ρ0′\rho_{0}' a radius for the local minimum of V∗−θ\mathcal{V}_{*}-\theta at ω1\omega_{1}, we get

V∗(ω1)−S0(ω1) ≤ V∗(ω)−S0(ω)\mathcal{V}_{*}(\omega_{1})-S_{0}(\omega_{1})\ \le\ \mathcal{V}_{*}(\omega)-S_{0}(\omega)

whenever ∥ω−ω1∥\lVert\omega-\omega_{1}\rVert is less than both ρ0′\rho_{0}' and ρ1′\rho_{1}'. Setting S=S0∘ΛS=S_{0}\circ\Lambda, we have S∈C2(H)S\in C^{2}(H), S(y)S(y) depends only on Λy\Lambda y, D2S(y)D^{2}S(y) is the constant form bv=(D2θ(ω1))Λ−2η1Πb_{v}=(D^{2}\theta(\omega_{1}))^{\Lambda}-2\eta_{1}\Pi with ∥bv−Y∥≤ε′+2η1\lVert b_{v}-Y\rVert\le\varepsilon'+2\eta_{1}, and ∣DS(y)−Λ♯Dθ(ω1)∣≤(∥D2θ(ω1)∥+2η1)∥Λy−ω1∥\bigl|DS(y)-\Lambda^{\sharp}D\theta(\omega_{1})\bigr|\le(\lVert D^{2}\theta(\omega_{1})\rVert+2\eta_{1})\lVert\Lambda y-\omega_{1}\rVert.

Step 5 (the fibre radius). By (iv) of Claim 3 and Euclidean Space and Real Matrices: Standing Notation (v), ∥D2χ(ζ1)∥≤∥X0∥+ε′≤6α+ε′\lVert D^{2}\chi(\zeta_{1})\rVert\le\lVert X_{0}\rVert+\varepsilon'\le6\alpha+\varepsilon', and likewise for θ\theta; put K=6α+ε′+2η1K=6\alpha+\varepsilon'+2\eta_{1}, so that the two gradient estimates of Step 4 hold with the factor KK. Let rr be a positive real number with

2r≤ρ0,2r≤ρ1,2r≤ρ0′,2r≤ρ1′,r≤1,Kr≤ε16,2∣α∣ r (D0+2)≤η016,2r\le\rho_{0},\quad 2r\le\rho_{1},\quad 2r\le\rho_{0}',\quad 2r\le\rho_{1}',\quad r\le1,\quad Kr\le\tfrac{\varepsilon}{16},\quad 2|\alpha|\,r\,(D_{0}+2)\le\tfrac{\eta_{0}}{16},

and such that

∣T0(ζ)−T0(ζ1)∣≤η016  whenever ∥ζ−ζ1∥≤r,∣S0(ω)−S0(ω1)∣≤η016  whenever ∥ω−ω1∥≤r.\bigl|T_{0}(\zeta)-T_{0}(\zeta_{1})\bigr|\le\tfrac{\eta_{0}}{16}\ \text{ whenever }\lVert\zeta-\zeta_{1}\rVert\le r, \qquad \bigl|S_{0}(\omega)-S_{0}(\omega_{1})\bigr|\le\tfrac{\eta_{0}}{16}\ \text{ whenever }\lVert\omega-\omega_{1}\rVert\le r .

Such an rr exists: the first seven conditions hold for every positive rr at most the least of the seven positive numbers

ρ02,ρ12,ρ0′2,ρ1′2,1,ε16K,η016 (2∣α∣(D0+2)+1),\tfrac{\rho_{0}}{2},\qquad\tfrac{\rho_{1}}{2},\qquad\tfrac{\rho_{0}'}{2},\qquad\tfrac{\rho_{1}'}{2},\qquad 1,\qquad\tfrac{\varepsilon}{16K},\qquad\tfrac{\eta_{0}}{16\,(2|\alpha|(D_{0}+2)+1)},

the sixth of which is defined because KK is positive; and for the last two it suffices, by the final estimate of Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iv), that r≤1r\le1 and (∥q∥+12∥M∥+∣η∣) r≤η016(\lVert q\rVert+\tfrac12\lVert M\rVert+|\eta|)\,r\le\tfrac{\eta_{0}}{16} for each of the two quadratics, since then ∥ζ−ζ1∥≤r≤1\lVert\zeta-\zeta_{1}\rVert\le r\le1 gives ∥ζ−ζ1∥2≤∥ζ−ζ1∥≤r\lVert\zeta-\zeta_{1}\rVert^{2}\le\lVert\zeta-\zeta_{1}\rVert\le r. Put

Au={ x∈A:∥Λx−ζ1∥≤r },Av={ y∈A:∥Λy−ω1∥≤r }.A_{u}=\{\,x\in A:\lVert\Lambda x-\zeta_{1}\rVert\le r\,\}, \qquad A_{v}=\{\,y\in A:\lVert\Lambda y-\omega_{1}\rVert\le r\,\}.

Step 6 (the auxiliary functions). Let Θu,Θv:A→R\Theta_{u},\Theta_{v}:A\to\mathbb{R} be given by Θu(x)=u^(x)−T(x)\Theta_{u}(x)=\hat{u}(x)-T(x) and Θv(y)=−v^(y)+S(y)\Theta_{v}(y)=-\hat{v}(y)+S(y), and put

Mu=U∗(ζ1)−T0(ζ1),Mv=−V∗(ω1)+S0(ω1).M_{u}=U^{*}(\zeta_{1})-T_{0}(\zeta_{1}),\qquad M_{v}=-\mathcal{V}_{*}(\omega_{1})+S_{0}(\omega_{1}).

(a) Upper bounds. Let x∈Aux\in A_{u}. Then u^(x)≤U(Λx)≤U∗(Λx)\hat{u}(x)\le U(\Lambda x)\le U^{*}(\Lambda x), by the definition of UU in Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes (i) and claim 1 of Properties of the Upper Semicontinuous Envelope; and T(x)=T0(Λx)T(x)=T_{0}(\Lambda x) with ∥Λx−ζ1∥≤r\lVert\Lambda x-\zeta_{1}\rVert\le r, which is less than both ρ0\rho_{0} and ρ1\rho_{1}. So Step 4 gives Θu(x)≤U∗(Λx)−T0(Λx)≤Mu\Theta_{u}(x)\le U^{*}(\Lambda x)-T_{0}(\Lambda x)\le M_{u}. Symmetrically Θv(y)≤Mv\Theta_{v}(y)\le M_{v} for every y∈Avy\in A_{v}, using −v^(y)≤−V(Λy)≤−V∗(Λy)-\hat{v}(y)\le-\mathcal{V}(\Lambda y)\le-\mathcal{V}_{*}(\Lambda y) (claim 2 of Properties of the Lower Semicontinuous Envelope, by Duality).

(b) Near-maximisers on a prescribed fibre neighbourhood. Let τ\tau and ss be positive with s≤rs\le r. Let s′s' be a positive number, at most ss, with ∣T0(ζ)−T0(ζ1)∣≤τ2\bigl|T_{0}(\zeta)-T_{0}(\zeta_{1})\bigr|\le\tfrac{\tau}{2} whenever ∥ζ−ζ1∥≤s′\lVert\zeta-\zeta_{1}\rVert\le s'; such an s′s' exists by the argument used for rr in Step 5. Applying Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes (iv) with ζ1\zeta_{1}, the radius s′s' and the accuracy τ2\tfrac{\tau}{2} gives x∈Ax\in A with ∥Λx−ζ1∥≤s′≤s≤r\lVert\Lambda x-\zeta_{1}\rVert\le s'\le s\le r, hence x∈Aux\in A_{u}, and U∗(ζ1)−τ2<u^(x)U^{*}(\zeta_{1})-\tfrac{\tau}{2}<\hat{u}(x). Since T(x)=T0(Λx)≤T0(ζ1)+τ2T(x)=T_{0}(\Lambda x)\le T_{0}(\zeta_{1})+\tfrac{\tau}{2},

Θu(x)=u^(x)−T0(Λx)>U∗(ζ1)−τ2−T0(ζ1)−τ2=Mu−τ.\Theta_{u}(x)=\hat{u}(x)-T_{0}(\Lambda x)>U^{*}(\zeta_{1})-\tfrac{\tau}{2}-T_{0}(\zeta_{1})-\tfrac{\tau}{2}=M_{u}-\tau .

Applying the same clause of Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes again, this time with ω1\omega_{1} in the role of ζ1\zeta_{1}, and using the second half of its conclusion (the one concerning v^\hat{v} and V∗\mathcal{V}_{*}) together with S0S_{0} in place of T0T_{0}, gives in the same way a y∈Avy\in A_{v} with ∥Λy−ω1∥≤s\lVert\Lambda y-\omega_{1}\rVert\le s and Mv−τ<Θv(y)M_{v}-\tau<\Theta_{v}(y). In particular AuA_{u} and AvA_{v} are nonempty.

(c) Closed superlevel sets. The functions gg, kk, TT and SS belong to C2(H)C^{2}(H): for TT and SS this is Step 4, and for gg note that

g(x)=−α⟨zˉ,x⟩+α⟨zˉ,xˉ⟩−α(N(x,x)−2⟨TNxˉ,x⟩+N(xˉ,xˉ)),g(x)=-\alpha\langle\bar{z},x\rangle+\alpha\langle\bar{z},\bar{x}\rangle-\alpha\Bigl(N(x,x)-2\langle T_{N}\bar{x},x\rangle+N(\bar{x},\bar{x})\Bigr),

by the bilinearity and symmetry of NN and claim 1 of The Bounded Symmetric Operator Represented by a Bounded Symmetric Bilinear Form on a Real Hilbert Space, which exhibits gg as a sum of an affine function and a scalar multiple of x↦12N(x,x)x\mapsto\tfrac12N(x,x); so claims 1 and 2 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C2C^2 and claims 2 and 3 of Constants, Sums, Scalar Multiples and Differences of Differentiable Functions on an Open Subset of a Real Inner Product Space give g∈C2(H)g\in C^{2}(H) with

Dg(x)=−αzˉ−2α TN(x−xˉ),D2g(x)=−2αN,Dg(x)=-\alpha\bar{z}-2\alpha\,T_{N}(x-\bar{x}),\qquad D^{2}g(x)=-2\alpha N ,

and likewise k∈C2(H)k\in C^{2}(H) with Dk(y)=αzˉ−2αTN(y−yˉ)Dk(y)=\alpha\bar{z}-2\alpha T_{N}(y-\bar{y}) and D2k(y)=−2αND^{2}k(y)=-2\alpha N. By claim 4 of The Bounded Symmetric Operator Represented by a Bounded Symmetric Bilinear Form on a Real Hilbert Space and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (iii), TNz=z−PzT_{N}z=z-Pz, so ∣TNz∣≤∣z∣|T_{N}z|\le|z|.

Members of C2(H)C^{2}(H) are differentiable on HH and hence continuous on HH, by The Classes C1C^1 and C2C^2 on an Open Subset of a Real Inner Product Space (ii) and Basic Properties of Differentiability on an Open Subset of a Real Inner Product Space (ii). Thus T−gT-g is continuous on HH, and Θu(x)=u(x)−(T(x)−g(x))\Theta_{u}(x)=u(x)-\bigl(T(x)-g(x)\bigr), so Θu\Theta_{u} has closed superlevel sets in HH as a function on AA, by claim 3 of Functions with Closed Superlevel Sets: Sequential Characterisation, Semicontinuity, Perturbation and Limits.

The restriction of Θu\Theta_{u} to AuA_{u} also has closed superlevel sets in HH. Indeed, let (xj)j∈N(x_{j})_{j\in\mathbb{N}} be a sequence in AuA_{u} converging to x∈Hx\in H and let t∈Rt\in\mathbb{R} satisfy t≤Θu(xj)t\le\Theta_{u}(x_{j}) for every jj. By claim 1 of Functions with Closed Superlevel Sets: Sequential Characterisation, Semicontinuity, Perturbation and Limits applied to Θu\Theta_{u} on AA we get x∈Ax\in A and t≤Θu(x)t\le\Theta_{u}(x). Moreover, for each jj,

∥Λx−ζ1∥≤∥Λx−Λxj∥+∥Λxj−ζ1∥≤∣x−xj∣+r,\lVert\Lambda x-\zeta_{1}\rVert\le\lVert\Lambda x-\Lambda x_{j}\rVert+\lVert\Lambda x_{j}-\zeta_{1}\rVert\le|x-x_{j}|+r ,

by Rn\mathbb{R}^n with the Euclidean Distance Is a Complete Metric Space with Coordinatewise Convergence and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (i); since ∣x−xj∣|x-x_{j}| is smaller than any prescribed positive number for suitable jj, Comparison of Real Numbers with Arbitrary Positive Slack gives ∥Λx−ζ1∥≤r\lVert\Lambda x-\zeta_{1}\rVert\le r, so x∈Aux\in A_{u}. By claim 1 of Functions with Closed Superlevel Sets: Sequential Characterisation, Semicontinuity, Perturbation and Limits again, in the converse direction, the restriction has closed superlevel sets in HH. The same argument applies to Θv\Theta_{v} on AvA_{v}.

Step 7 (the perturbed maxima). Let λ\lambda be the lesser of r8\tfrac{r}{8} and 11, and let μ\mu be a positive real with

2μ≤ε16,16μλ≤ε16,8μλ2≤η016,2\mu\le\tfrac{\varepsilon}{16},\qquad 16\mu\lambda\le\tfrac{\varepsilon}{16},\qquad 8\mu\lambda^{2}\le\tfrac{\eta_{0}}{16},

which exists as the least of three positive numbers of the required form. Then 4λ≤r24\lambda\le\tfrac{r}{2}.

By (b) with τ=μλ2\tau=\mu\lambda^{2} and s=r4s=\tfrac{r}{4} there is x0∈Aux_{0}\in A_{u} with ∥Λx0−ζ1∥≤r4\lVert\Lambda x_{0}-\zeta_{1}\rVert\le\tfrac{r}{4} and Mu−μλ2<Θu(x0)M_{u}-\mu\lambda^{2}<\Theta_{u}(x_{0}). By (a), MuM_{u} is an upper bound for the values of Θu\Theta_{u} on AuA_{u}, so the least upper bound of those values is at most Θu(x0)+μλ2\Theta_{u}(x_{0})+\mu\lambda^{2}. Hence A Perturbed Maximum Principle of Borwein-Preiss Type in a Real Hilbert Space applies to AuA_{u}, Θu\Theta_{u}, μ\mu, λ\lambda and x0x_{0}, and provides two points, written here c1∈Hc_{1}\in H and x1∈Aux_{1}\in A_{u} — they are the points called yˉ\bar{y} and xˉ\bar{x} in that theorem, and are unrelated to the point yˉ\bar{y} of the present lemma — such that

∣x1−x0∣≤4λ,∣x1−c1∣≤8λ,|x_{1}-x_{0}|\le4\lambda,\qquad |x_{1}-c_{1}|\le8\lambda,

the function on AuA_{u} with value Θu(x)−μ∣x−c1∣2\Theta_{u}(x)-\mu|x-c_{1}|^{2} at xx attains a sequentially strict maximum on AuA_{u} at x1x_{1} (claim 2 there), and the least upper bound of the values of Θu\Theta_{u} on AuA_{u} is at most Θu(x1)+2μλ2\Theta_{u}(x_{1})+2\mu\lambda^{2} (claim 3 there). Combining the last bound with Mu−μλ2<Θu(x0)M_{u}-\mu\lambda^{2}<\Theta_{u}(x_{0}) gives

Mu−3μλ2<Θu(x1).M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}).

Also

∥Λx1−ζ1∥≤∥Λ(x1−x0)∥+∥Λx0−ζ1∥≤∣x1−x0∣+r4≤4λ+r4≤r2+r4<r.\lVert\Lambda x_{1}-\zeta_{1}\rVert\le\lVert\Lambda(x_{1}-x_{0})\rVert+\lVert\Lambda x_{0}-\zeta_{1}\rVert\le|x_{1}-x_{0}|+\tfrac{r}{4}\le4\lambda+\tfrac{r}{4}\le\tfrac{r}{2}+\tfrac{r}{4}<r .

The same construction on the vv side provides c2∈Hc_{2}\in H and y1∈Avy_{1}\in A_{v} with ∣y1−c2∣≤8λ|y_{1}-c_{2}|\le8\lambda, with Θv−μ∣⋅−c2∣2\Theta_{v}-\mu|\cdot-c_{2}|^{2} attaining a sequentially strict maximum on AvA_{v} at y1y_{1}, with Mv−3μλ2<Θv(y1)M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) and with ∥Λy1−ω1∥<r\lVert\Lambda y_{1}-\omega_{1}\rVert<r.

Step 8 (the test functions and the local extrema). Define φ,ψ:H→R\varphi,\psi:H\to\mathbb{R} by

φ(x)=T(x)−g(x)+μ ∣x−c1∣2,ψ(y)=S(y)+k(y)−μ ∣y−c2∣2,\varphi(x)=T(x)-g(x)+\mu\,|x-c_{1}|^{2}, \qquad \psi(y)=S(y)+k(y)-\mu\,|y-c_{2}|^{2},

so that, for x,y∈Ax,y\in A,

u(x)−φ(x)=Θu(x)−μ∣x−c1∣2,v(y)−ψ(y)=−(Θv(y)−μ∣y−c2∣2).u(x)-\varphi(x)=\Theta_{u}(x)-\mu|x-c_{1}|^{2}, \qquad v(y)-\psi(y)=-\Bigl(\Theta_{v}(y)-\mu|y-c_{2}|^{2}\Bigr).

Put ρ2=r−∥Λx1−ζ1∥\rho_{2}=r-\lVert\Lambda x_{1}-\zeta_{1}\rVert, positive by Step 7. If x∈Ax\in A and ∣x−x1∣<ρ2|x-x_{1}|<\rho_{2} then

∥Λx−ζ1∥≤∥Λ(x−x1)∥+∥Λx1−ζ1∥≤∣x−x1∣+∥Λx1−ζ1∥<r,\lVert\Lambda x-\zeta_{1}\rVert\le\lVert\Lambda(x-x_{1})\rVert+\lVert\Lambda x_{1}-\zeta_{1}\rVert\le|x-x_{1}|+\lVert\Lambda x_{1}-\zeta_{1}\rVert<r,

so x∈Aux\in A_{u} and hence, the sequentially strict maximum of Step 7 being in particular a maximum on AuA_{u} (clause 1 of Sequentially Strict Maxima and Minima on a Subset of a Metric Space (i)),

u(x)−φ(x)=Θu(x)−μ∣x−c1∣2≤Θu(x1)−μ∣x1−c1∣2=u(x1)−φ(x1).u(x)-\varphi(x)=\Theta_{u}(x)-\mu|x-c_{1}|^{2}\le\Theta_{u}(x_{1})-\mu|x_{1}-c_{1}|^{2}=u(x_{1})-\varphi(x_{1}).

Thus u−φu-\varphi has a local maximum at x1x_{1} relative to AA. The same argument on the vv side shows that Θv−μ∣⋅−c2∣2\Theta_{v}-\mu|\cdot-c_{2}|^{2} has a local maximum at y1y_{1} relative to AA, hence that v−ψv-\psi, being its additive inverse there, has a local minimum at y1y_{1} relative to AA.

By Step 4, Step 6(c) and claim 3 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C2C^2 (applied with 2μ2\mu in the role of the coefficient), each of TT, gg, SS, kk and the two squared-distance terms belongs to C2(H)C^{2}(H); so φ,ψ∈C2(H)\varphi,\psi\in C^{2}(H) by claims 2 and 4 of Constants, Sums, Scalar Multiples and Differences of Differentiable Functions on an Open Subset of a Real Inner Product Space, with

Dφ(x1)=DT(x1)−Dg(x1)+2μ(x1−c1),D2φ(x1)=bu+2αN+2μI,D\varphi(x_{1})=DT(x_{1})-Dg(x_{1})+2\mu(x_{1}-c_{1}), \qquad D^{2}\varphi(x_{1})=b_{u}+2\alpha N+2\mu I, Dψ(y1)=DS(y1)+Dk(y1)−2μ(y1−c2),D2ψ(y1)=bv−2αN−2μI.D\psi(y_{1})=DS(y_{1})+Dk(y_{1})-2\mu(y_{1}-c_{2}), \qquad D^{2}\psi(y_{1})=b_{v}-2\alpha N-2\mu I .

Step 9 (the localisation). Write Ξ(x,y)=u^(x)−v^(y)−α2∥Λx−Λy∥2\Xi(x,y)=\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2} for x,y∈Ax,y\in A, and M1=Ξ(xˉ,yˉ)M_{1}=\Xi(\bar{x},\bar{y}); by Claim 2, Φ(x,y)≥Ξ(x,y)−α2∣zˉ∣2\Phi(x,y)\ge\Xi(x,y)-\tfrac{\alpha}{2}|\bar{z}|^{2} and M1=M0+α2∣zˉ∣2M_{1}=M_{0}+\tfrac{\alpha}{2}|\bar{z}|^{2}. Since T(x1)=T0(Λx1)T(x_{1})=T_{0}(\Lambda x_{1}) and S(y1)=S0(Λy1)S(y_{1})=S_{0}(\Lambda y_{1}),

Ξ(x1,y1)=Θu(x1)+Θv(y1)+T0(Λx1)−S0(Λy1)−α2∥Λx1−Λy1∥2.\Xi(x_{1},y_{1})=\Theta_{u}(x_{1})+\Theta_{v}(y_{1})+T_{0}(\Lambda x_{1})-S_{0}(\Lambda y_{1})-\tfrac{\alpha}{2}\lVert\Lambda x_{1}-\Lambda y_{1}\rVert^{2}.

By Step 3 and Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes (iii) (through Claim 3),

Mu+Mv=U∗(ζ1)−V∗(ω1)−T0(ζ1)+S0(ω1)>U∗(ζˉ)−V∗(ωˉ)−2ε′−T0(ζ1)+S0(ω1),M_{u}+M_{v}=U^{*}(\zeta_{1})-\mathcal{V}_{*}(\omega_{1})-T_{0}(\zeta_{1})+S_{0}(\omega_{1}) >U^{*}(\bar{\zeta})-\mathcal{V}_{*}(\bar{\omega})-2\varepsilon'-T_{0}(\zeta_{1})+S_{0}(\omega_{1}),

and U∗(ζˉ)−V∗(ωˉ)=u^(xˉ)−v^(yˉ)=M1+α2D02U^{*}(\bar{\zeta})-\mathcal{V}_{*}(\bar{\omega})=\hat{u}(\bar{x})-\hat{v}(\bar{y})=M_{1}+\tfrac{\alpha}{2}D_{0}^{2}. With Mu−3μλ2<Θu(x1)M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}) and Mv−3μλ2<Θv(y1)M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) from Step 7, this gives

Ξ(x1,y1)>M1+α2D02−2ε′−6μλ2+[T0(Λx1)−T0(ζ1)]−[S0(Λy1)−S0(ω1)]−α2∥Λx1−Λy1∥2.\Xi(x_{1},y_{1})>M_{1}+\tfrac{\alpha}{2}D_{0}^{2}-2\varepsilon'-6\mu\lambda^{2} +\bigl[T_{0}(\Lambda x_{1})-T_{0}(\zeta_{1})\bigr]-\bigl[S_{0}(\Lambda y_{1})-S_{0}(\omega_{1})\bigr]-\tfrac{\alpha}{2}\lVert\Lambda x_{1}-\Lambda y_{1}\rVert^{2}.

By Step 7 we have ∥Λx1−ζ1∥≤r\lVert\Lambda x_{1}-\zeta_{1}\rVert\le r and ∥Λy1−ω1∥≤r\lVert\Lambda y_{1}-\omega_{1}\rVert\le r, so each of the two bracketed terms has absolute value at most η016\tfrac{\eta_{0}}{16} by Step 5, and therefore each is at least −η016-\tfrac{\eta_{0}}{16} by claim 3 of Properties of the Absolute Value in an Ordered Field. Next, ∥ζˉ−Λx1∥≤∥ζˉ−ζ1∥+∥ζ1−Λx1∥<ε′+r\lVert\bar{\zeta}-\Lambda x_{1}\rVert\le\lVert\bar{\zeta}-\zeta_{1}\rVert+\lVert\zeta_{1}-\Lambda x_{1}\rVert<\varepsilon'+r and similarly ∥ωˉ−Λy1∥<ε′+r\lVert\bar{\omega}-\Lambda y_{1}\rVert<\varepsilon'+r; so Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions (vi), applied with (ζˉ,ωˉ)(\bar{\zeta},\bar{\omega}) and (Λx1,Λy1)(\Lambda x_{1},\Lambda y_{1}), gives ∥Λx1−Λy1∥≤D0+2(ε′+r)≤D0+4\lVert\Lambda x_{1}-\Lambda y_{1}\rVert\le D_{0}+2(\varepsilon'+r)\le D_{0}+4 (as ε′≤1\varepsilon'\le1 and r≤1r\le1) and hence

∣α2D02−α2∥Λx1−Λy1∥2∣≤∣α∣2 (2D0+4)⋅2(ε′+r)=2∣α∣ (ε′+r) (D0+2)≤η016+η016,\Bigl|\tfrac{\alpha}{2}D_{0}^{2}-\tfrac{\alpha}{2}\lVert\Lambda x_{1}-\Lambda y_{1}\rVert^{2}\Bigr| \le\tfrac{|\alpha|}{2}\,(2D_{0}+4)\cdot2(\varepsilon'+r) =2|\alpha|\,(\varepsilon'+r)\,(D_{0}+2)\le\tfrac{\eta_{0}}{16}+\tfrac{\eta_{0}}{16},

by Steps 2 and 5. Since also 2ε′≤η082\varepsilon'\le\tfrac{\eta_{0}}{8} and 6μλ2≤η0166\mu\lambda^{2}\le\tfrac{\eta_{0}}{16}, we conclude

Ξ(x1,y1)>M1−η08−η016−η016−η016−η016−η016 ≥ M1−η0,\Xi(x_{1},y_{1})>M_{1}-\tfrac{\eta_{0}}{8}-\tfrac{\eta_{0}}{16}-\tfrac{\eta_{0}}{16}-\tfrac{\eta_{0}}{16}-\tfrac{\eta_{0}}{16}-\tfrac{\eta_{0}}{16}\ \ge\ M_{1}-\eta_{0},

and therefore Φ(x1,y1)≥Ξ(x1,y1)−α2∣zˉ∣2>M1−η0−α2∣zˉ∣2=M0−η0\Phi(x_{1},y_{1})\ge\Xi(x_{1},y_{1})-\tfrac{\alpha}{2}|\bar{z}|^{2}>M_{1}-\eta_{0}-\tfrac{\alpha}{2}|\bar{z}|^{2}=M_{0}-\eta_{0}. By Step 1,

∣x1−xˉ∣<ε1≤ε,∣y1−yˉ∣<ε1≤ε,∣u(x1)−u(xˉ)∣<ε1≤ε,∣v(y1)−v(yˉ)∣<ε1≤ε,|x_{1}-\bar{x}|<\varepsilon_{1}\le\varepsilon,\quad |y_{1}-\bar{y}|<\varepsilon_{1}\le\varepsilon,\quad |u(x_{1})-u(\bar{x})|<\varepsilon_{1}\le\varepsilon,\quad |v(y_{1})-v(\bar{y})|<\varepsilon_{1}\le\varepsilon,

which are four of the eight required inequalities.

Step 10 (the gradients and Hessians). By Step 8, Step 6(c) and Claim 3,

Dφ(x1)−p=(DT(x1)−Λ♯Dχ(ζ1))+Λ♯(Dχ(ζ1)−p0)+2α TN(x1−xˉ)+2μ(x1−c1),D\varphi(x_{1})-p=\Bigl(DT(x_{1})-\Lambda^{\sharp}D\chi(\zeta_{1})\Bigr)+\Lambda^{\sharp}\bigl(D\chi(\zeta_{1})-p_{0}\bigr)+2\alpha\,T_{N}(x_{1}-\bar{x})+2\mu(x_{1}-c_{1}),

because −Dg(x1)=αzˉ+2αTN(x1−xˉ)-Dg(x_{1})=\alpha\bar{z}+2\alpha T_{N}(x_{1}-\bar{x}), because Λ♯\Lambda^{\sharp} is linear, and because p=Λ♯p0+αzˉp=\Lambda^{\sharp}p_{0}+\alpha\bar{z}. The four terms are estimated in turn: the first has norm at most K∥Λx1−ζ1∥≤Kr≤ε16K\lVert\Lambda x_{1}-\zeta_{1}\rVert\le Kr\le\tfrac{\varepsilon}{16} by Steps 4, 5 and 7; the second has norm ∥Dχ(ζ1)−p0∥<ε′≤ε16\lVert D\chi(\zeta_{1})-p_{0}\rVert<\varepsilon'\le\tfrac{\varepsilon}{16}, since ∣Λ♯ξ∣=∥ξ∥|\Lambda^{\sharp}\xi|=\lVert\xi\rVert; the third has norm at most 2α∣x1−xˉ∣<2αε1≤ε42\alpha|x_{1}-\bar{x}|<2\alpha\varepsilon_{1}\le\tfrac{\varepsilon}{4} by ∣TNz∣≤∣z∣|T_{N}z|\le|z|, Step 9 and ε1≤ε8α\varepsilon_{1}\le\tfrac{\varepsilon}{8\alpha}; and the fourth has norm 2μ∣x1−c1∣≤16μλ≤ε162\mu|x_{1}-c_{1}|\le16\mu\lambda\le\tfrac{\varepsilon}{16} by Step 7. By the triangle inequality (claim 1 of The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity),

∣Dφ(x1)−p∣≤ε16+ε16+ε4+ε16<ε.\bigl|D\varphi(x_{1})-p\bigr|\le\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{4}+\tfrac{\varepsilon}{16}<\varepsilon .

For the Hessian, D2φ(x1)−(X+2αN)=(bu−X)+2μID^{2}\varphi(x_{1})-(X+2\alpha N)=(b_{u}-X)+2\mu I by Step 8, so by claims 1 and 3 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity, Step 4 and Step 7,

∥D2φ(x1)−(X+2αN)∥≤∥bu−X∥+2μ∥I∥≤(ε′+2η1)+2μ≤ε16+ε16+ε16<ε.\bigl\lVert D^{2}\varphi(x_{1})-(X+2\alpha N)\bigr\rVert\le\lVert b_{u}-X\rVert+2\mu\lVert I\rVert\le(\varepsilon'+2\eta_{1})+2\mu\le\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{16}<\varepsilon .

On the vv side, Dk(y1)=αzˉ−2αTN(y1−yˉ)Dk(y_{1})=\alpha\bar{z}-2\alpha T_{N}(y_{1}-\bar{y}), so

Dψ(y1)−p=(DS(y1)−Λ♯Dθ(ω1))+Λ♯(Dθ(ω1)−p0)−2α TN(y1−yˉ)−2μ(y1−c2),D\psi(y_{1})-p=\Bigl(DS(y_{1})-\Lambda^{\sharp}D\theta(\omega_{1})\Bigr)+\Lambda^{\sharp}\bigl(D\theta(\omega_{1})-p_{0}\bigr)-2\alpha\,T_{N}(y_{1}-\bar{y})-2\mu(y_{1}-c_{2}),

and the same four estimates, with ∥Λy1−ω1∥≤r\lVert\Lambda y_{1}-\omega_{1}\rVert\le r and ∣y1−yˉ∣<ε1|y_{1}-\bar{y}|<\varepsilon_{1} in place of their counterparts, give ∣Dψ(y1)−p∣<ε|D\psi(y_{1})-p|<\varepsilon. Finally D2ψ(y1)−(Y−2αN)=(bv−Y)−2μID^{2}\psi(y_{1})-(Y-2\alpha N)=(b_{v}-Y)-2\mu I, whose norm is at most (ε′+2η1)+2μ<ε(\varepsilon'+2\eta_{1})+2\mu<\varepsilon as before.

This establishes all eight inequalities and completes the proof of Claim 4, hence of clause 1 and of the lemma.

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