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Proof of Lions' Lemma on a Hilbert Space: Test Data and Form Bounds at a Sequentially Strict Maximum of a Quadratically Penalised Difference

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· 31,521 chars · 28 deps · depth 24 Reason: Proof of Lions' lemma on a Hilbert space, independent of the source, which states the result without proof. The tail of the penalty is split off by an inequality that decouples the two variables and is exact at the maximum point; the resulting functional is carried to Euclidean space by fibre suprema, where the published finite-dimensional lemma applies; the Euclidean test data are lifted back by the perturbed maximum principle, and the pair of lifted points is localised by the localisation lemma.

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 MS(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=ΛΛP=\Lambda^{\sharp}\Lambda, Λx=Pxx\lVert\Lambda x\rVert=|Px|\le|x|, Λξ=ξ|\Lambda^{\sharp}\xi|=\lVert\xi\rVert, x2=Π(x,x)+N(x,x)|x|^{2}=\Pi(x,x)+N(x,x) and N(x,x)=xPx2N(x,x)=|x-Px|^{2}, so that xPxx|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=(xˉyˉ)P(xˉyˉ),M_{0}=\Phi(\bar{x},\bar{y}),\qquad \bar{z}=(\bar{x}-\bar{y})-P(\bar{x}-\bar{y}),

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

g(x)=αzˉ,xxˉαN(xxˉ,xxˉ),k(y)=αzˉ,yyˉαN(yyˉ,yyˉ).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 §maximum, 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,yHx,y\in H,

α2N(xy,xy)  α2zˉ2+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)α4zˉ2g(x)\le\tfrac{\alpha}{4}|\bar{z}|^{2} and k(y)α4zˉ2k(y)\le\tfrac{\alpha}{4}|\bar{z}|^{2} for all x,yHx,y\in H.

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

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

because (xy)=(xxˉ)(yyˉ)+(xˉyˉ)(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 §tail,

N(xy,xy)=ab+zˉ2,N(xxˉ,xxˉ)=a2,N(yyˉ,yyˉ)=b2,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)=zPz,wN(z,w)=\langle z-Pz,w\rangle there together with the first,

zˉ,xxˉ=N(xˉyˉ,xxˉ)=zˉ,a,zˉ,yyˉ=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 §expansion applied twice, and by Elementary Identities in a Real Inner Product Space §bilinear,

ab+zˉ2=ab2+2ab,zˉ+zˉ2=ab2+2zˉ,a2zˉ,b+zˉ2,|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 ab2=a22a,b+b2|a-b|^{2}=|a|^{2}-2\langle a,b\rangle+|b|^{2} while 0a+b2=a2+2a,b+b20\le|a+b|^{2}=|a|^{2}+2\langle a,b\rangle+|b|^{2}, so 2a,ba2+b2-2\langle a,b\rangle\le|a|^{2}+|b|^{2} and therefore ab22a2+2b2|a-b|^{2}\le2|a|^{2}+2|b|^{2}. Hence

N(xy,xy)zˉ2+2zˉ,a2zˉ,b+2a2+2b2.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(xy,xy)  α2zˉ2αzˉ,a+αzˉ,bαa2αb2=α2zˉ2+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(xˉyˉ,xˉyˉ)=zˉ2N(\bar{x}-\bar{y},\bar{x}-\bar{y})=|\bar{z}|^{2}, and both sides equal α2zˉ2-\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,azˉ,azˉa-\langle\bar{z},a\rangle\le|\langle\bar{z},a\rangle|\le|\bar{z}|\,|a|, so g(x)αzˉaαa2g(x)\le\alpha|\bar{z}||a|-\alpha|a|^{2} by claim 5 of Elementary Arithmetic in an Ordered Field. Since 0α(azˉ2)2=αa2αzˉa+α4zˉ20\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 αzˉaαa2α4zˉ2\alpha|\bar{z}||a|-\alpha|a|^{2}\le\tfrac{\alpha}{4}|\bar{z}|^{2}, whence g(x)α4zˉ2g(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^:AR\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)α2ΛxΛy2α2zˉ2  Φ(x,y)for all x,yA,\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)α2ΛxΛy2  u^(xˉ)v^(yˉ)α2ΛxˉΛyˉ2for all x,yA.\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 §coordinates and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail, ΛxΛy=Λ(xy)\lVert\Lambda x-\Lambda y\rVert=\lVert\Lambda(x-y)\rVert and xy2=Λ(xy)2+N(xy,xy)|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)α2ΛxΛy2α2N(xy,xy)  u(x)+g(x)(v(y)k(y))α2ΛxΛy2α2zˉ2,\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)α2ΛxΛy2Φ(x,y)+α2zˉ2M0+α2zˉ2,\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)α2ΛxˉΛyˉ2\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+α4zˉ2\hat{u}(x)\le C_{u}+\tfrac{\alpha}{4}|\bar{z}|^{2} and v^(y)=v(y)+k(y)Cv+α4zˉ2-\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}, UU^{*}, 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 §maximum, UU^{*} is upper semicontinuous on Rm\mathbb{R}^{m}, V\mathcal{V}_{*} is lower semicontinuous on Rm\mathbb{R}^{m}, and

U(ζ)V(ω)α2ζω2  U(ζˉ)V(ωˉ)α2ζˉωˉ2for all ζ,ωRm;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 §values, 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, and CkC^k Maps are Continuous, 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 UU^{*} 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(ζˉωˉ)p_{0}=\alpha(\bar{\zeta}-\bar{\omega}), we obtain X0,Y0S(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 UU^{*} 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,ηRm\xi,\eta\in\mathbb{R}^{m},

3α(ξ2+η2)ξ(X0ξ)η(Y0η)3αξη2-3\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) X0Y0X_{0}\preceq Y_{0} (clause 4 there); and (iv) X06α\lVert X_{0}\rVert\le6\alpha and Y06α\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 §forms. 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 MΛM\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 0Λ(zw)zw0\le\lVert\Lambda(z-w)\rVert\le|z-w|, two applications of claim 5 of Elementary Arithmetic in an Ordered Field give ΛzΛw2=Λ(zw)2zw2\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 Λz2+Λw2z2+w2\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(z2+w2)3α(Λz2+Λw2)-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 ζˉωˉ=Λ(xˉyˉ)\bar{\zeta}-\bar{\omega}=\Lambda(\bar{x}-\bar{y}), so that by the linearity of Λ\Lambda^{\sharp} and P=ΛΛP=\Lambda^{\sharp}\Lambda,

Λp0=αP(xˉyˉ),whencep=α(xˉyˉ)=αP(xˉyˉ)+αzˉ=Λp0+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 εR\varepsilon\in\mathbb{R} be positive. We produce x1,y1Ax_{1},y_{1}\in A and φ,ψC2(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

x1xˉ<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, y1yˉ<ε,v(y1)v(yˉ)<ε,Dψ(y1)p<ε,D2ψ(y1)(Y2αN)<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 §above and Quadruple Approximable by Test Data on a Subset of a Real Inner Product Space §below.

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 §localisation provides a positive η0R\eta_{0}\in\mathbb{R} such that every (x,y)A×A(x,y)\in A\times A with M0η0<Φ(x,y)M_{0}-\eta_{0}<\Phi(x,y) satisfies

xxˉ<ε1,yyˉ<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=ζˉωˉD_{0}=\lVert\bar{\zeta}-\bar{\omega}\rVert. Let ε\varepsilon' be a positive real number with

ε1,εε16,εη016,2αε(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(2α(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 2η1ε162\eta_{1}\le\tfrac{\varepsilon}{16}.

Step 3 (the Euclidean test data). By (i) of Claim 3 and Quadruple Approximable by Test-Function Data §above, applied with the accuracy ε\varepsilon', there are ζ1Rm\zeta_{1}\in\mathbb{R}^{m} and a function χ:RmR\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 §below, there are ω1Rm\omega_{1}\in\mathbb{R}^{m} and θ:RmR\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 §majorant 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)(ζζ1)+12(ζζ1)(D2χ(ζ1)(ζζ1))+η1ζζ12T_{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 ζζ1<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 ζζ1\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=T0ΛT=T_{0}\circ\Lambda. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §quadratic, TC2(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+2η1Π,b_{u}=\bigl(D^{2}\chi(\zeta_{1})\bigr)^{\Lambda}+2\eta_{1}\,\Pi ,

and DT(x)ΛDχ(ζ1)(D2χ(ζ1)+2η1)Λxζ1\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 xHx\in H. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §forms and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail, together with claims 1 and 3 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity,

buX(D2χ(ζ1)X0)Λ+2η1Πε+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 §majorant 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 ωω1<ρ1\lVert\omega-\omega_{1}\rVert<\rho_{1}'; with ρ0\rho_{0}' a radius for the local minimum of Vθ\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 ωω1\lVert\omega-\omega_{1}\rVert is less than both ρ0\rho_{0}' and ρ1\rho_{1}'. Setting S=S0ΛS=S_{0}\circ\Lambda, we have SC2(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))Λ2η1Πb_{v}=(D^{2}\theta(\omega_{1}))^{\Lambda}-2\eta_{1}\Pi with bvYε+2η1\lVert b_{v}-Y\rVert\le\varepsilon'+2\eta_{1}, and DS(y)ΛDθ(ω1)(D2θ(ω1)+2η1)Λyω1\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 Real Matrices, Symmetric Matrices and the Semidefinite Ordering: Standing Notation §norm, D2χ(ζ1)X0+ε6α+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

2rρ0,2rρ1,2rρ0,2rρ1,r1,Krε16,2αr(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 ζζ1r,S0(ω)S0(ω1)η016  whenever ωω1r.\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,ρ02,ρ12,1,ε16K,η016(2α(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 §quadratic, that r1r\le1 and (q+12M+η)rη016(\lVert q\rVert+\tfrac12\lVert M\rVert+|\eta|)\,r\le\tfrac{\eta_{0}}{16} for each of the two quadratics, since then ζζ1r1\lVert\zeta-\zeta_{1}\rVert\le r\le1 gives ζζ12ζζ1r\lVert\zeta-\zeta_{1}\rVert^{2}\le\lVert\zeta-\zeta_{1}\rVert\le r. Put

Au={xA:Λxζ1r},Av={yA:Λyω1r}.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:AR\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 xAux\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 §defined and claim 1 of Properties of the Upper Semicontinuous Envelope; and T(x)=T0(Λx)T(x)=T_{0}(\Lambda x) with Λxζ1r\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 yAvy\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 srs\le r. Let ss' 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 ζζ1s\lVert\zeta-\zeta_{1}\rVert\le s'; such an ss' exists by the argument used for rr in Step 5. Applying Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes §approximation with ζ1\zeta_{1}, the radius ss' and the accuracy τ2\tfrac{\tau}{2} gives xAx\in A with Λxζ1ssr\lVert\Lambda x-\zeta_{1}\rVert\le s'\le s\le r, hence xAux\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)τ2T0(ζ1)τ2=Muτ.\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 yAvy\in A_{v} with Λyω1s\lVert\Lambda y-\omega_{1}\rVert\le s and Mvτ<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)=αzˉ,x+αzˉ,xˉα(N(x,x)2TNxˉ,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 x12N(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 gC2(H)g\in C^{2}(H) with

Dg(x)=αzˉ2αTN(xxˉ),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 kC2(H)k\in C^{2}(H) with Dk(y)=αzˉ2αTN(yyˉ)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 §tail, TNz=zPzT_{N}z=z-Pz, so TNzz|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 §c2 and Basic Properties of Differentiability on an Open Subset of a Real Inner Product Space §continuous. Thus TgT-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)jN(x_{j})_{j\in\mathbb{N}} be a sequence in AuA_{u} converging to xHx\in H and let tRt\in\mathbb{R} satisfy tΘu(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 xAx\in A and tΘu(x)t\le\Theta_{u}(x). Moreover, for each jj,

Λxζ1ΛxΛxj+Λxjζ1xxj+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 Euclidean Distance is a Metric on Rn\mathbb{R}^n and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §coordinates; since xxj|x-x_{j}| is smaller than any prescribed positive number for suitable jj, Comparison of Real Numbers with Arbitrary Positive Slack gives Λxζ1r\lVert\Lambda x-\zeta_{1}\rVert\le r, so xAux\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

2με16,16μλε16,8μλ2η016,2\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 4λr24\lambda\le\tfrac{r}{2}.

By (b) with τ=μλ2\tau=\mu\lambda^{2} and s=r4s=\tfrac{r}{4} there is x0Aux_{0}\in A_{u} with Λx0ζ1r4\lVert\Lambda x_{0}-\zeta_{1}\rVert\le\tfrac{r}{4} and Muμλ2<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 c1Hc_{1}\in H and x1Aux_{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

x1x04λ,x1c18λ,|x_{1}-x_{0}|\le4\lambda,\qquad |x_{1}-c_{1}|\le8\lambda,

the function on AuA_{u} with value Θu(x)μxc12\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 Muμλ2<Θu(x0)M_{u}-\mu\lambda^{2}<\Theta_{u}(x_{0}) gives

Mu3μλ2<Θu(x1).M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}).

Also

Λx1ζ1Λ(x1x0)+Λx0ζ1x1x0+r44λ+r4r2+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 c2Hc_{2}\in H and y1Avy_{1}\in A_{v} with y1c28λ|y_{1}-c_{2}|\le8\lambda, with Θvμc22\Theta_{v}-\mu|\cdot-c_{2}|^{2} attaining a sequentially strict maximum on AvA_{v} at y1y_{1}, with Mv3μλ2<Θv(y1)M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) and with Λy1ω1<r\lVert\Lambda y_{1}-\omega_{1}\rVert<r.

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

φ(x)=T(x)g(x)+μxc12,ψ(y)=S(y)+k(y)μyc22,\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,yAx,y\in A,

u(x)φ(x)=Θu(x)μxc12,v(y)ψ(y)=(Θv(y)μyc22).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=rΛx1ζ1\rho_{2}=r-\lVert\Lambda x_{1}-\zeta_{1}\rVert, positive by Step 7. If xAx\in A and xx1<ρ2|x-x_{1}|<\rho_{2} then

Λxζ1Λ(xx1)+Λx1ζ1xx1+Λx1ζ1<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 xAux\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 §maximum),

u(x)φ(x)=Θu(x)μxc12Θu(x1)μx1c12=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 uφu-\varphi has a local maximum at x1x_{1} relative to AA. The same argument on the vv side shows that Θvμc22\Theta_{v}-\mu|\cdot-c_{2}|^{2} has a local maximum at y1y_{1} relative to AA, hence that vψv-\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,ψC2(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(x1c1),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(y1c2),D2ψ(y1)=bv2αN2μI.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)α2ΛxΛy2\Xi(x,y)=\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2} for x,yAx,y\in A, and M1=Ξ(xˉ,yˉ)M_{1}=\Xi(\bar{x},\bar{y}); by Claim 2, Φ(x,y)Ξ(x,y)α2zˉ2\Phi(x,y)\ge\Xi(x,y)-\tfrac{\alpha}{2}|\bar{z}|^{2} and M1=M0+α2zˉ2M_{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)α2Λx1Λy12.\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 §values (through Claim 3),

Mu+Mv=U(ζ1)V(ω1)T0(ζ1)+S0(ω1)>U(ζˉ)V(ωˉ)2εT0(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 Mu3μλ2<Θu(x1)M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}) and Mv3μλ2<Θv(y1)M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) from Step 7, this gives

Ξ(x1,y1)>M1+α2D022ε6μλ2+[T0(Λx1)T0(ζ1)][S0(Λy1)S0(ω1)]α2Λx1Λy12.\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 Λx1ζ1r\lVert\Lambda x_{1}-\zeta_{1}\rVert\le r and Λy1ω1r\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, ζˉΛx1ζˉζ1+ζ1Λx1<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 ωˉΛy1<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 §stability, applied with (ζˉ,ωˉ)(\bar{\zeta},\bar{\omega}) and (Λx1,Λy1)(\Lambda x_{1},\Lambda y_{1}), gives Λx1Λy1D0+2(ε+r)D0+4\lVert\Lambda x_{1}-\Lambda y_{1}\rVert\le D_{0}+2(\varepsilon'+r)\le D_{0}+4 (as ε1\varepsilon'\le1 and r1r\le1) and hence

α2D02α2Λx1Λy12α2(2D0+4)2(ε+r)=2α(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 2εη082\varepsilon'\le\tfrac{\eta_{0}}{8} and 6μλ2η0166\mu\lambda^{2}\le\tfrac{\eta_{0}}{16}, we conclude

Ξ(x1,y1)>M1η08η016η016η016η016η016  M1η0,\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)α2zˉ2>M1η0α2zˉ2=M0η0\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,

x1xˉ<ε1ε,y1yˉ<ε1ε,u(x1)u(xˉ)<ε1ε,v(y1)v(yˉ)<ε1ε,|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)ΛDχ(ζ1))+Λ(Dχ(ζ1)p0)+2αTN(x1xˉ)+2μ(x1c1),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(x1xˉ)-Dg(x_{1})=\alpha\bar{z}+2\alpha T_{N}(x_{1}-\bar{x}), because Λ\Lambda^{\sharp} is linear, and because p=Λp0+αzˉp=\Lambda^{\sharp}p_{0}+\alpha\bar{z}. The four terms are estimated in turn: the first has norm at most KΛx1ζ1Krε16K\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<εε16\lVert D\chi(\zeta_{1})-p_{0}\rVert<\varepsilon'\le\tfrac{\varepsilon}{16}, since Λξ=ξ|\Lambda^{\sharp}\xi|=\lVert\xi\rVert; the third has norm at most 2αx1xˉ<2αε1ε42\alpha|x_{1}-\bar{x}|<2\alpha\varepsilon_{1}\le\tfrac{\varepsilon}{4} by TNzz|T_{N}z|\le|z|, Step 9 and ε1ε8α\varepsilon_{1}\le\tfrac{\varepsilon}{8\alpha}; and the fourth has norm 2μx1c116μλε162\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)pε16+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)=(buX)+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)buX+2μI(ε+2η1)+2με16+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)=αzˉ2αTN(y1yˉ)Dk(y_{1})=\alpha\bar{z}-2\alpha T_{N}(y_{1}-\bar{y}), so

Dψ(y1)p=(DS(y1)ΛDθ(ω1))+Λ(Dθ(ω1)p0)2αTN(y1yˉ)2μ(y1c2),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 Λy1ω1r\lVert\Lambda y_{1}-\omega_{1}\rVert\le r and y1yˉ<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)(Y2αN)=(bvY)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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