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 , Λ ♯ \Lambda^{\sharp} Λ ♯ , P P P , the forms M Λ M^{\Lambda} M Λ for M ∈ S ( m ) M\in\mathcal{S}(m) M ∈ S ( m ) , the projection form Π \Pi Π and the tail form N N N be those determined by e e e 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 Λ and Λ ♯ \Lambda^{\sharp} Λ ♯ are linear, P = Λ ♯ Λ P=\Lambda^{\sharp}\Lambda P = Λ ♯ Λ , ∥ Λ x ∥ = ∣ P x ∣ ≤ ∣ x ∣ \lVert\Lambda x\rVert=|Px|\le|x| ∥ Λ x ∥ = ∣ P x ∣ ≤ ∣ x ∣ , ∣ Λ ♯ ξ ∣ = ∥ ξ ∥ |\Lambda^{\sharp}\xi|=\lVert\xi\rVert ∣ Λ ♯ ξ ∣ = ∥ ξ ∥ , ∣ x ∣ 2 = Π ( x , x ) + N ( x , x ) |x|^{2}=\Pi(x,x)+N(x,x) ∣ x ∣ 2 = Π ( x , x ) + N ( x , x ) and N ( x , x ) = ∣ x − P x ∣ 2 N(x,x)=|x-Px|^{2} N ( x , x ) = ∣ x − P x ∣ 2 , so that ∣ x − P x ∣ ≤ ∣ x ∣ |x-Px|\le|x| ∣ x − P x ∣ ≤ ∣ x ∣ . Since ∣ e 1 ∣ = 1 |e_{1}|=1 ∣ e 1 ∣ = 1 we have H ≠ { 0 H } H\ne\{0_{H}\} H = { 0 H } , so ∥ I ∥ = 1 \lVert I\rVert=1 ∥ I ∥ = 1 by claim 3 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity . Write
M 0 = Φ ( x ˉ , y ˉ ) , z ˉ = ( x ˉ − y ˉ ) − P ( x ˉ − y ˉ ) , M_{0}=\Phi(\bar{x},\bar{y}),\qquad \bar{z}=(\bar{x}-\bar{y})-P(\bar{x}-\bar{y}), M 0 = Φ ( x ˉ , y ˉ ) , z ˉ = ( x ˉ − y ˉ ) − P ( x ˉ − y ˉ ) ,
and let g , k : H → R g,k:H\to\mathbb{R} g , k : H → R be given by
g ( x ) = − α ⟨ z ˉ , x − x ˉ ⟩ − α N ( x − x ˉ , x − x ˉ ) , k ( y ) = α ⟨ z ˉ , y − y ˉ ⟩ − α N ( y − y ˉ , y − y ˉ ) . 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}). g ( x ) = − α ⟨ z ˉ , x − x ˉ ⟩ − α N ( x − x ˉ , x − x ˉ ) , k ( y ) = α ⟨ z ˉ , y − y ˉ ⟩ − α N ( y − y ˉ , y − y ˉ ) .
By clause 1 of Sequentially Strict Maxima and Minima on a Subset of a Metric Space §maximum , Φ ( x , y ) ≤ M 0 \Phi(x,y)\le M_{0} Φ ( x , y ) ≤ M 0 for all ( x , y ) ∈ A × A (x,y)\in A\times A ( x , y ) ∈ A × A . Every component of e e e lies in A A A , so A A A is nonempty.
Claim 1 (splitting off the tail of the penalty). For all x , y ∈ H x,y\in H x , y ∈ H ,
− α 2 N ( x − y , x − y ) ≥ − α 2 ∣ z ˉ ∣ 2 + g ( x ) + k ( y ) , -\tfrac{\alpha}{2}\,N(x-y,x-y)\ \ge\ -\tfrac{\alpha}{2}\,|\bar{z}|^{2}+g(x)+k(y), − 2 α N ( x − y , x − y ) ≥ − 2 α ∣ z ˉ ∣ 2 + g ( x ) + k ( y ) ,
with equality when x = x ˉ x=\bar{x} x = x ˉ and y = y ˉ y=\bar{y} y = y ˉ ; moreover g ( x ) ≤ α 4 ∣ z ˉ ∣ 2 g(x)\le\tfrac{\alpha}{4}|\bar{z}|^{2} g ( x ) ≤ 4 α ∣ z ˉ ∣ 2 and k ( y ) ≤ α 4 ∣ z ˉ ∣ 2 k(y)\le\tfrac{\alpha}{4}|\bar{z}|^{2} k ( y ) ≤ 4 α ∣ z ˉ ∣ 2 for all x , y ∈ H x,y\in H x , y ∈ H .
Proof. Put a = ( x − x ˉ ) − P ( x − x ˉ ) a=(x-\bar{x})-P(x-\bar{x}) a = ( x − x ˉ ) − P ( x − x ˉ ) and b = ( y − y ˉ ) − P ( y − y ˉ ) b=(y-\bar{y})-P(y-\bar{y}) b = ( y − y ˉ ) − P ( y − y ˉ ) . Since P P P is linear,
( x − y ) − P ( x − y ) = a − b + z ˉ , (x-y)-P(x-y)=a-b+\bar{z}, ( x − y ) − P ( x − y ) = a − b + z ˉ ,
because ( x − y ) = ( x − x ˉ ) − ( y − y ˉ ) + ( x ˉ − y ˉ ) (x-y)=(x-\bar{x})-(y-\bar{y})+(\bar{x}-\bar{y}) ( x − y ) = ( x − x ˉ ) − ( y − y ˉ ) + ( x ˉ − y ˉ ) . By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail ,
N ( x − y , x − y ) = ∣ a − b + z ˉ ∣ 2 , N ( x − x ˉ , x − x ˉ ) = ∣ a ∣ 2 , N ( y − y ˉ , y − y ˉ ) = ∣ 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}, N ( x − y , x − y ) = ∣ a − b + z ˉ ∣ 2 , N ( x − x ˉ , x − x ˉ ) = ∣ a ∣ 2 , N ( y − y ˉ , y − y ˉ ) = ∣ b ∣ 2 ,
and, using the second expression N ( z , w ) = ⟨ z − P z , w ⟩ N(z,w)=\langle z-Pz,w\rangle N ( z , w ) = ⟨ z − P z , w ⟩ there together with the first,
⟨ z ˉ , x − x ˉ ⟩ = N ( x ˉ − y ˉ , x − x ˉ ) = ⟨ z ˉ , a ⟩ , ⟨ z ˉ , y − y ˉ ⟩ = ⟨ z ˉ , 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 . ⟨ z ˉ , x − x ˉ ⟩ = N ( x ˉ − y ˉ , x − x ˉ ) = ⟨ z ˉ , a ⟩ , ⟨ z ˉ , y − y ˉ ⟩ = ⟨ z ˉ , b ⟩ .
By Elementary Identities in a Real Inner Product Space §expansion applied twice, and by Elementary Identities in a Real Inner Product Space §bilinear ,
∣ a − b + z ˉ ∣ 2 = ∣ a − b ∣ 2 + 2 ⟨ a − b , z ˉ ⟩ + ∣ z ˉ ∣ 2 = ∣ a − b ∣ 2 + 2 ⟨ z ˉ , a ⟩ − 2 ⟨ z ˉ , b ⟩ + ∣ z ˉ ∣ 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}, ∣ a − b + z ˉ ∣ 2 = ∣ a − b ∣ 2 + 2 ⟨ a − b , z ˉ ⟩ + ∣ z ˉ ∣ 2 = ∣ a − b ∣ 2 + 2 ⟨ z ˉ , a ⟩ − 2 ⟨ z ˉ , b ⟩ + ∣ z ˉ ∣ 2 ,
and ∣ a − b ∣ 2 = ∣ a ∣ 2 − 2 ⟨ a , b ⟩ + ∣ b ∣ 2 |a-b|^{2}=|a|^{2}-2\langle a,b\rangle+|b|^{2} ∣ a − b ∣ 2 = ∣ a ∣ 2 − 2 ⟨ a , b ⟩ + ∣ b ∣ 2 while 0 ≤ ∣ a + b ∣ 2 = ∣ a ∣ 2 + 2 ⟨ a , b ⟩ + ∣ b ∣ 2 0\le|a+b|^{2}=|a|^{2}+2\langle a,b\rangle+|b|^{2} 0 ≤ ∣ a + b ∣ 2 = ∣ a ∣ 2 + 2 ⟨ a , b ⟩ + ∣ b ∣ 2 , so − 2 ⟨ a , b ⟩ ≤ ∣ a ∣ 2 + ∣ b ∣ 2 -2\langle a,b\rangle\le|a|^{2}+|b|^{2} − 2 ⟨ a , b ⟩ ≤ ∣ a ∣ 2 + ∣ b ∣ 2 and therefore ∣ a − b ∣ 2 ≤ 2 ∣ a ∣ 2 + 2 ∣ b ∣ 2 |a-b|^{2}\le2|a|^{2}+2|b|^{2} ∣ a − b ∣ 2 ≤ 2∣ a ∣ 2 + 2∣ b ∣ 2 . Hence
N ( x − y , x − y ) ≤ ∣ z ˉ ∣ 2 + 2 ⟨ z ˉ , a ⟩ − 2 ⟨ z ˉ , 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}. N ( x − y , x − y ) ≤ ∣ z ˉ ∣ 2 + 2 ⟨ z ˉ , a ⟩ − 2 ⟨ z ˉ , b ⟩ + 2∣ a ∣ 2 + 2∣ b ∣ 2 .
Multiplying by the positive number α 2 \tfrac{\alpha}{2} 2 α (claim 5 of Elementary Arithmetic in an Ordered Field ) and reversing the sign (claim 4 of Elementary Order Arithmetic in an Ordered Field ) gives
− α 2 N ( x − y , x − y ) ≥ − α 2 ∣ z ˉ ∣ 2 − α ⟨ z ˉ , a ⟩ + α ⟨ z ˉ , b ⟩ − α ∣ a ∣ 2 − α ∣ b ∣ 2 = − α 2 ∣ z ˉ ∣ 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), − 2 α N ( x − y , x − y ) ≥ − 2 α ∣ z ˉ ∣ 2 − α ⟨ z ˉ , a ⟩ + α ⟨ z ˉ , b ⟩ − α ∣ a ∣ 2 − α ∣ b ∣ 2 = − 2 α ∣ z ˉ ∣ 2 + g ( x ) + k ( y ) ,
by the identities displayed above. If x = x ˉ x=\bar{x} x = x ˉ and y = y ˉ y=\bar{y} y = y ˉ then a = b = 0 H a=b=0_{H} a = b = 0 H , so g ( x ˉ ) = 0 g(\bar{x})=0 g ( x ˉ ) = 0 , k ( y ˉ ) = 0 k(\bar{y})=0 k ( y ˉ ) = 0 and N ( x ˉ − y ˉ , x ˉ − y ˉ ) = ∣ z ˉ ∣ 2 N(\bar{x}-\bar{y},\bar{x}-\bar{y})=|\bar{z}|^{2} N ( x ˉ − y ˉ , x ˉ − y ˉ ) = ∣ z ˉ ∣ 2 , and both sides equal − α 2 ∣ z ˉ ∣ 2 -\tfrac{\alpha}{2}|\bar{z}|^{2} − 2 α ∣ z ˉ ∣ 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 − ⟨ z ˉ , a ⟩ ≤ ∣ ⟨ z ˉ , a ⟩ ∣ ≤ ∣ z ˉ ∣ ∣ a ∣ -\langle\bar{z},a\rangle\le|\langle\bar{z},a\rangle|\le|\bar{z}|\,|a| − ⟨ z ˉ , a ⟩ ≤ ∣ ⟨ z ˉ , a ⟩ ∣ ≤ ∣ z ˉ ∣ ∣ a ∣ , so g ( x ) ≤ α ∣ z ˉ ∣ ∣ a ∣ − α ∣ a ∣ 2 g(x)\le\alpha|\bar{z}||a|-\alpha|a|^{2} g ( x ) ≤ α ∣ z ˉ ∣∣ a ∣ − α ∣ a ∣ 2 by claim 5 of Elementary Arithmetic in an Ordered Field . Since 0 ≤ α ( ∣ a ∣ − ∣ z ˉ ∣ 2 ) 2 = α ∣ a ∣ 2 − α ∣ z ˉ ∣ ∣ a ∣ + α 4 ∣ z ˉ ∣ 2 0\le\alpha\bigl(|a|-\tfrac{|\bar{z}|}{2}\bigr)^{2}=\alpha|a|^{2}-\alpha|\bar{z}||a|+\tfrac{\alpha}{4}|\bar{z}|^{2} 0 ≤ α ( ∣ a ∣ − 2 ∣ z ˉ ∣ ) 2 = α ∣ a ∣ 2 − α ∣ z ˉ ∣∣ a ∣ + 4 α ∣ z ˉ ∣ 2 , we get α ∣ z ˉ ∣ ∣ a ∣ − α ∣ a ∣ 2 ≤ α 4 ∣ z ˉ ∣ 2 \alpha|\bar{z}||a|-\alpha|a|^{2}\le\tfrac{\alpha}{4}|\bar{z}|^{2} α ∣ z ˉ ∣∣ a ∣ − α ∣ a ∣ 2 ≤ 4 α ∣ z ˉ ∣ 2 , whence g ( x ) ≤ α 4 ∣ z ˉ ∣ 2 g(x)\le\tfrac{\alpha}{4}|\bar{z}|^{2} g ( x ) ≤ 4 α ∣ z ˉ ∣ 2 . The same computation with b b b in place of a a a bounds k k k . This proves Claim 1.
Claim 2 (the decoupled functional). Let u ^ , v ^ : A → R \hat{u},\hat{v}:A\to\mathbb{R} u ^ , v ^ : A → R be given by u ^ ( x ) = u ( x ) + g ( x ) \hat{u}(x)=u(x)+g(x) u ^ ( x ) = u ( x ) + g ( x ) and v ^ ( y ) = v ( y ) − k ( y ) \hat{v}(y)=v(y)-k(y) v ^ ( y ) = v ( y ) − k ( y ) . Then the set of values of u ^ \hat{u} u ^ is bounded above and that of v ^ \hat{v} v ^ is bounded below;
u ^ ( x ) − v ^ ( y ) − α 2 ∥ Λ x − Λ y ∥ 2 − α 2 ∣ z ˉ ∣ 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, u ^ ( x ) − v ^ ( y ) − 2 α ∥ Λ x − Λ y ∥ 2 − 2 α ∣ z ˉ ∣ 2 ≤ Φ ( x , y ) for all x , y ∈ A ,
with equality when x = x ˉ x=\bar{x} x = x ˉ , y = y ˉ y=\bar{y} y = y ˉ ; and
u ^ ( x ) − v ^ ( y ) − α 2 ∥ Λ x − Λ y ∥ 2 ≤ u ^ ( x ˉ ) − v ^ ( y ˉ ) − α 2 ∥ Λ x ˉ − Λ y ˉ ∥ 2 for 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 . u ^ ( x ) − v ^ ( y ) − 2 α ∥ Λ x − Λ y ∥ 2 ≤ u ^ ( x ˉ ) − v ^ ( y ˉ ) − 2 α ∥ Λ x ˉ − Λ y ˉ ∥ 2 for all x , y ∈ 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 , ∥ Λ x − Λ y ∥ = ∥ Λ ( x − y ) ∥ \lVert\Lambda x-\Lambda y\rVert=\lVert\Lambda(x-y)\rVert ∥ Λ x − Λ y ∥ = ∥ Λ ( x − y )∥ 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) ∣ x − y ∣ 2 = ∥ Λ ( x − y ) ∥ 2 + N ( x − y , x − y ) . Hence, by Claim 1,
Φ ( x , y ) = u ( x ) − v ( y ) − α 2 ∥ Λ x − Λ y ∥ 2 − α 2 N ( x − y , x − y ) ≥ u ( x ) + g ( x ) − ( v ( y ) − k ( y ) ) − α 2 ∥ Λ x − Λ y ∥ 2 − α 2 ∣ z ˉ ∣ 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}, Φ ( x , y ) = u ( x ) − v ( y ) − 2 α ∥ Λ x − Λ y ∥ 2 − 2 α N ( x − y , x − y ) ≥ u ( x ) + g ( x ) − ( v ( y ) − k ( y ) ) − 2 α ∥ Λ x − Λ y ∥ 2 − 2 α ∣ z ˉ ∣ 2 ,
which is the first display; equality at ( x ˉ , y ˉ ) (\bar{x},\bar{y}) ( x ˉ , y ˉ ) follows from the equality case of Claim 1. For the second display, the first one and Φ ( x , y ) ≤ M 0 \Phi(x,y)\le M_{0} Φ ( x , y ) ≤ M 0 give
u ^ ( x ) − v ^ ( y ) − α 2 ∥ Λ x − Λ y ∥ 2 ≤ Φ ( x , y ) + α 2 ∣ z ˉ ∣ 2 ≤ M 0 + α 2 ∣ z ˉ ∣ 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}, u ^ ( x ) − v ^ ( y ) − 2 α ∥ Λ x − Λ y ∥ 2 ≤ Φ ( x , y ) + 2 α ∣ z ˉ ∣ 2 ≤ M 0 + 2 α ∣ z ˉ ∣ 2 ,
and by the equality case the right-hand side equals u ^ ( x ˉ ) − v ^ ( y ˉ ) − α 2 ∥ Λ x ˉ − Λ y ˉ ∥ 2 \hat{u}(\bar{x})-\hat{v}(\bar{y})-\tfrac{\alpha}{2}\lVert\Lambda\bar{x}-\Lambda\bar{y}\rVert^{2} u ^ ( x ˉ ) − v ^ ( y ˉ ) − 2 α ∥ Λ x ˉ − Λ y ˉ ∥ 2 . Finally, let C u C_{u} C u be an upper bound for the values of u u u and C v C_{v} C v one for the values of − v -v − v ; by Claim 1, u ^ ( x ) ≤ C u + α 4 ∣ z ˉ ∣ 2 \hat{u}(x)\le C_{u}+\tfrac{\alpha}{4}|\bar{z}|^{2} u ^ ( x ) ≤ C u + 4 α ∣ z ˉ ∣ 2 and − v ^ ( y ) = − v ( y ) + k ( y ) ≤ C v + α 4 ∣ z ˉ ∣ 2 -\hat{v}(y)=-v(y)+k(y)\le C_{v}+\tfrac{\alpha}{4}|\bar{z}|^{2} − v ^ ( y ) = − v ( y ) + k ( y ) ≤ C v + 4 α ∣ z ˉ ∣ 2 , so the values of v ^ \hat{v} 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 A A A , e e e , u ^ \hat{u} u ^ , v ^ \hat{v} v ^ , α \alpha α , x ˉ \bar{x} x ˉ , y ˉ \bar{y} y ˉ . Let U U U , V \mathcal{V} V , U ∗ U^{*} U ∗ , V ∗ \mathcal{V}_{*} V ∗ , ζ ˉ = Λ x ˉ \bar{\zeta}=\Lambda\bar{x} ζ ˉ = Λ x ˉ and ω ˉ = Λ y ˉ \bar{\omega}=\Lambda\bar{y} ω ˉ = Λ y ˉ be as there. By Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes §maximum , U ∗ U^{*} U ∗ is upper semicontinuous on R m \mathbb{R}^{m} R m , V ∗ \mathcal{V}_{*} V ∗ is lower semicontinuous on R m \mathbb{R}^{m} R m , and
U ∗ ( ζ ) − V ∗ ( ω ) − α 2 ∥ ζ − ω ∥ 2 ≤ U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) − α 2 ∥ ζ ˉ − ω ˉ ∥ 2 for all ζ , ω ∈ R m ; 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}; U ∗ ( ζ ) − V ∗ ( ω ) − 2 α ∥ ζ − ω ∥ 2 ≤ U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) − 2 α ∥ ζ ˉ − ω ˉ ∥ 2 for all ζ , ω ∈ R m ;
and by Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes §values , U ∗ ( ζ ˉ ) = u ^ ( x ˉ ) U^{*}(\bar{\zeta})=\hat{u}(\bar{x}) U ∗ ( ζ ˉ ) = u ^ ( x ˉ ) and V ∗ ( ω ˉ ) = v ^ ( y ˉ ) \mathcal{V}_{*}(\bar{\omega})=\hat{v}(\bar{y}) V ∗ ( ω ˉ ) = v ^ ( y ˉ ) .
The set R m \mathbb{R}^{m} R m is open in R m \mathbb{R}^{m} R m by claim 1 of Euclidean Space is Open in Itself, and C k C^k C k Maps are Continuous , so Ishii's Lemma: Test Data and Matrix Bounds at a Maximum of a Quadratically Penalised Difference applies with m m m in the role of n n n , with Ω = R m \Omega=\mathbb{R}^{m} Ω = R m , with U ∗ U^{*} U ∗ and V ∗ \mathcal{V}_{*} V ∗ in the roles of u u u and v v v , with α \alpha α , and with ζ ˉ \bar{\zeta} ζ ˉ and ω ˉ \bar{\omega} ω ˉ in the roles of the two points; its local hypothesis holds with δ = 1 \delta=1 δ = 1 because the displayed inequality holds for all ζ , ω \zeta,\omega ζ , ω . Writing p 0 = α ( ζ ˉ − ω ˉ ) p_{0}=\alpha(\bar{\zeta}-\bar{\omega}) p 0 = α ( ζ ˉ − ω ˉ ) , we obtain X 0 , Y 0 ∈ S ( m ) X_{0},Y_{0}\in\mathcal{S}(m) X 0 , Y 0 ∈ S ( m ) such that
(i) the quadruple ( ζ ˉ , U ∗ ( ζ ˉ ) , p 0 , X 0 ) (\bar{\zeta},U^{*}(\bar{\zeta}),p_{0},X_{0}) ( ζ ˉ , U ∗ ( ζ ˉ ) , p 0 , X 0 ) is approximable by test data from above for U ∗ U^{*} U ∗ and ( ω ˉ , V ∗ ( ω ˉ ) , p 0 , Y 0 ) (\bar{\omega},\mathcal{V}_{*}(\bar{\omega}),p_{0},Y_{0}) ( ω ˉ , V ∗ ( ω ˉ ) , p 0 , Y 0 ) is approximable by test data from below for V ∗ \mathcal{V}_{*} V ∗ , the open set being R m \mathbb{R}^{m} R m in both cases (clause 1 there); (ii) for all ξ , η ∈ R m \xi,\eta\in\mathbb{R}^{m} ξ , η ∈ R m ,
− 3 α ( ∥ ξ ∥ 2 + ∥ η ∥ 2 ) ≤ ξ ⋅ ( X 0 ξ ) − η ⋅ ( Y 0 η ) ≤ 3 α ∥ 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} − 3 α ( ∥ ξ ∥ 2 + ∥ η ∥ 2 ) ≤ ξ ⋅ ( X 0 ξ ) − η ⋅ ( Y 0 η ) ≤ 3 α ∥ ξ − η ∥ 2
(clause 3 there); (iii) X 0 ⪯ Y 0 X_{0}\preceq Y_{0} X 0 ⪯ Y 0 (clause 4 there); and (iv) ∥ X 0 ∥ ≤ 6 α \lVert X_{0}\rVert\le6\alpha ∥ X 0 ∥ ≤ 6 α and ∥ Y 0 ∥ ≤ 6 α \lVert Y_{0}\rVert\le6\alpha ∥ Y 0 ∥ ≤ 6 α (clause 5 there).
Put X = X 0 Λ X=X_{0}^{\Lambda} X = X 0 Λ and Y = Y 0 Λ Y=Y_{0}^{\Lambda} Y = Y 0 Λ , elements of S y m ( H ) \mathrm{Sym}(H) 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 M Λ ( z , w ) = M Λ ( P z , P w ) M^{\Lambda}(z,w)=M^{\Lambda}(Pz,Pw) M Λ ( z , w ) = M Λ ( P z , Pw ) of that clause, clause 4 follows from (iv) and the bound ∥ M Λ ∥ ≤ ∥ M ∥ \lVert M^{\Lambda}\rVert\le\lVert M\rVert ∥ M Λ ∥ ≤ ∥ M ∥ there, and clause 3 follows from (iii) and the order transfer there. For clause 2, apply (ii) with ξ = Λ z \xi=\Lambda z ξ = Λ z and η = Λ w \eta=\Lambda w η = Λ w , so that ξ ⋅ ( X 0 ξ ) = X ( z , z ) \xi\cdot(X_{0}\xi)=X(z,z) ξ ⋅ ( X 0 ξ ) = X ( z , z ) and η ⋅ ( Y 0 η ) = Y ( w , w ) \eta\cdot(Y_{0}\eta)=Y(w,w) η ⋅ ( Y 0 η ) = Y ( w , w ) . Since 0 ≤ ∥ Λ ( z − w ) ∥ ≤ ∣ z − w ∣ 0\le\lVert\Lambda(z-w)\rVert\le|z-w| 0 ≤ ∥ Λ ( z − w )∥ ≤ ∣ z − w ∣ , two applications of claim 5 of Elementary Arithmetic in an Ordered Field give ∥ Λ z − Λ w ∥ 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} ∥ Λ z − Λ w ∥ 2 = ∥ Λ ( z − w ) ∥ 2 ≤ ∣ z − w ∣ 2 , and multiplying by the nonnegative 3 α 3\alpha 3 α gives the upper bound of clause 2. Likewise ∥ Λ z ∥ 2 + ∥ Λ w ∥ 2 ≤ ∣ z ∣ 2 + ∣ w ∣ 2 \lVert\Lambda z\rVert^{2}+\lVert\Lambda w\rVert^{2}\le|z|^{2}+|w|^{2} ∥ Λ z ∥ 2 + ∥ Λ w ∥ 2 ≤ ∣ z ∣ 2 + ∣ w ∣ 2 , so multiplying by 3 α 3\alpha 3 α and reversing the sign gives − 3 α ( ∣ z ∣ 2 + ∣ w ∣ 2 ) ≤ − 3 α ( ∥ Λ z ∥ 2 + ∥ Λ w ∥ 2 ) -3\alpha(|z|^{2}+|w|^{2})\le-3\alpha(\lVert\Lambda z\rVert^{2}+\lVert\Lambda w\rVert^{2}) − 3 α ( ∣ z ∣ 2 + ∣ w ∣ 2 ) ≤ − 3 α (∥ Λ z ∥ 2 + ∥ Λ w ∥ 2 ) , which with (ii) gives the lower bound.
We record for later use that ζ ˉ − ω ˉ = Λ ( x ˉ − y ˉ ) \bar{\zeta}-\bar{\omega}=\Lambda(\bar{x}-\bar{y}) ζ ˉ − ω ˉ = Λ ( x ˉ − y ˉ ) , so that by the linearity of Λ ♯ \Lambda^{\sharp} Λ ♯ and P = Λ ♯ Λ P=\Lambda^{\sharp}\Lambda P = Λ ♯ Λ ,
Λ ♯ p 0 = α P ( x ˉ − y ˉ ) , whence p = α ( x ˉ − y ˉ ) = α P ( x ˉ − y ˉ ) + α z ˉ = Λ ♯ p 0 + α z ˉ . \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}. Λ ♯ p 0 = α P ( x ˉ − y ˉ ) , whence p = α ( x ˉ − y ˉ ) = α P ( x ˉ − y ˉ ) + α z ˉ = Λ ♯ p 0 + α z ˉ .
This proves Claim 3.
Claim 4 (clause 1). Let ε ∈ R \varepsilon\in\mathbb{R} ε ∈ R be positive. We produce x 1 , y 1 ∈ A x_{1},y_{1}\in A x 1 , y 1 ∈ A and φ , ψ ∈ C 2 ( H ) \varphi,\psi\in C^{2}(H) φ , ψ ∈ C 2 ( H ) such that the function on A A A with value u ( x ) − φ ( x ) u(x)-\varphi(x) u ( x ) − φ ( x ) at x x x has a local maximum at x 1 x_{1} x 1 relative to A A A , the function on A A A with value v ( y ) − ψ ( y ) v(y)-\psi(y) v ( y ) − ψ ( y ) at y y y has a local minimum at y 1 y_{1} y 1 relative to A A A , and
∣ x 1 − x ˉ ∣ < ε , ∣ u ( x 1 ) − u ( x ˉ ) ∣ < ε , ∣ D φ ( x 1 ) − p ∣ < ε , ∥ D 2 φ ( x 1 ) − ( X + 2 α N ) ∥ < 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, ∣ x 1 − x ˉ ∣ < ε , ∣ u ( x 1 ) − u ( x ˉ ) ∣ < ε , D φ ( x 1 ) − p < ε , D 2 φ ( x 1 ) − ( X + 2 α N ) < ε ,
∣ y 1 − y ˉ ∣ < ε , ∣ v ( y 1 ) − v ( y ˉ ) ∣ < ε , ∣ D ψ ( y 1 ) − p ∣ < ε , ∥ D 2 ψ ( y 1 ) − ( Y − 2 α N ) ∥ < 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 . ∣ y 1 − y ˉ ∣ < ε , ∣ v ( y 1 ) − v ( y ˉ ) ∣ < ε , D ψ ( y 1 ) − p < ε , D 2 ψ ( y 1 ) − ( Y − 2 α N ) < ε .
Since ε \varepsilon ε 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 ε 1 \varepsilon_{1} ε 1 be the lesser of ε \varepsilon ε and ε 8 α \tfrac{\varepsilon}{8\alpha} 8 α ε , positive because it is one of them. The function u u u and the function − v -v − v have closed superlevel sets in H H H , A A A is nonempty, and Φ \Phi Φ attains a sequentially strict maximum on A × A A\times A A × A at ( x ˉ , y ˉ ) (\bar{x},\bar{y}) ( x ˉ , y ˉ ) , so Localisation at a Sequentially Strict Maximum of a Quadratically Penalised Difference §localisation provides a positive η 0 ∈ R \eta_{0}\in\mathbb{R} η 0 ∈ R such that every ( x , y ) ∈ A × A (x,y)\in A\times A ( x , y ) ∈ A × A with M 0 − η 0 < Φ ( x , y ) M_{0}-\eta_{0}<\Phi(x,y) M 0 − η 0 < Φ ( x , y ) satisfies
∣ x − x ˉ ∣ < ε 1 , ∣ y − y ˉ ∣ < ε 1 , ∣ u ( x ) − u ( x ˉ ) ∣ < ε 1 , ∣ v ( y ) − v ( y ˉ ) ∣ < ε 1 . |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}. ∣ x − x ˉ ∣ < ε 1 , ∣ y − y ˉ ∣ < ε 1 , ∣ u ( x ) − u ( x ˉ ) ∣ < ε 1 , ∣ v ( y ) − v ( y ˉ ) ∣ < ε 1 .
Step 2 (accuracy of the Euclidean data). Put D 0 = ∥ ζ ˉ − ω ˉ ∥ D_{0}=\lVert\bar{\zeta}-\bar{\omega}\rVert D 0 = ∥ ζ ˉ − ω ˉ ∥ . Let ε ′ \varepsilon' ε ′ be a positive real number with
ε ′ ≤ 1 , ε ′ ≤ ε 16 , ε ′ ≤ η 0 16 , 2 ∣ α ∣ ε ′ ( D 0 + 2 ) ≤ η 0 16 , \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}, ε ′ ≤ 1 , ε ′ ≤ 16 ε , ε ′ ≤ 16 η 0 , 2∣ α ∣ ε ′ ( D 0 + 2 ) ≤ 16 η 0 ,
which exists: the first three are satisfied by the least of 1 1 1 , ε 16 \tfrac{\varepsilon}{16} 16 ε and η 0 16 \tfrac{\eta_{0}}{16} 16 η 0 , and the fourth by any positive number at most η 0 16 ( 2 ∣ α ∣ ( D 0 + 2 ) + 1 ) \tfrac{\eta_{0}}{16\,(2|\alpha|(D_{0}+2)+1)} 16 ( 2∣ α ∣ ( D 0 + 2 ) + 1 ) η 0 , so the least of these four positive numbers serves. Let η 1 \eta_{1} η 1 be a positive real with 2 η 1 ≤ ε 16 2\eta_{1}\le\tfrac{\varepsilon}{16} 2 η 1 ≤ 16 ε .
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' ε ′ , there are ζ 1 ∈ R m \zeta_{1}\in\mathbb{R}^{m} ζ 1 ∈ R m and a function χ : R m → R \chi:\mathbb{R}^{m}\to\mathbb{R} χ : R m → R of class C 2 C^{2} C 2 on R m \mathbb{R}^{m} R m such that the function with value U ∗ ( ζ ) − χ ( ζ ) U^{*}(\zeta)-\chi(\zeta) U ∗ ( ζ ) − χ ( ζ ) at ζ \zeta ζ has a local maximum at ζ 1 \zeta_{1} ζ 1 relative to R m \mathbb{R}^{m} R m and
d E ( ζ 1 , ζ ˉ ) < ε ′ , ∣ U ∗ ( ζ 1 ) − U ∗ ( ζ ˉ ) ∣ < ε ′ , ∥ D χ ( ζ 1 ) − p 0 ∥ < ε ′ , d S ( m ) ( D 2 χ ( ζ 1 ) , X 0 ) < 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' . d E ( ζ 1 , ζ ˉ ) < ε ′ , ∣ U ∗ ( ζ 1 ) − U ∗ ( ζ ˉ ) ∣ < ε ′ , ∥ Dχ ( ζ 1 ) − p 0 ∥ < ε ′ , d S ( m ) ( D 2 χ ( ζ 1 ) , X 0 ) < ε ′ .
Likewise, by Quadruple Approximable by Test-Function Data §below , there are ω 1 ∈ R m \omega_{1}\in\mathbb{R}^{m} ω 1 ∈ R m and θ : R m → R \theta:\mathbb{R}^{m}\to\mathbb{R} θ : R m → R of class C 2 C^{2} C 2 on R m \mathbb{R}^{m} R m such that the function with value V ∗ ( ω ) − θ ( ω ) \mathcal{V}_{*}(\omega)-\theta(\omega) V ∗ ( ω ) − θ ( ω ) at ω \omega ω has a local minimum at ω 1 \omega_{1} ω 1 relative to R m \mathbb{R}^{m} R m and the four analogous inequalities hold with ω 1 , θ , V ∗ , ω ˉ , Y 0 \omega_{1},\theta,\mathcal{V}_{*},\bar{\omega},Y_{0} ω 1 , θ , V ∗ , ω ˉ , Y 0 in place of ζ 1 , χ , U ∗ , ζ ˉ , X 0 \zeta_{1},\chi,U^{*},\bar{\zeta},X_{0} ζ 1 , χ , U ∗ , ζ ˉ , 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 = R m \Omega=\mathbb{R}^{m} Ω = R m , with χ \chi χ , ζ 1 \zeta_{1} ζ 1 and the positive η 1 \eta_{1} η 1 : the associated quadratic
T 0 ( ζ ) = χ ( ζ 1 ) + D χ ( ζ 1 ) ⋅ ( ζ − ζ 1 ) + 1 2 ( ζ − ζ 1 ) ⋅ ( D 2 χ ( ζ 1 ) ( ζ − ζ 1 ) ) + η 1 ∥ ζ − ζ 1 ∥ 2 T_{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} T 0 ( ζ ) = χ ( ζ 1 ) + Dχ ( ζ 1 ) ⋅ ( ζ − ζ 1 ) + 2 1 ( ζ − ζ 1 ) ⋅ ( D 2 χ ( ζ 1 ) ( ζ − ζ 1 ) ) + η 1 ∥ ζ − ζ 1 ∥ 2
satisfies T 0 ( ζ 1 ) = χ ( ζ 1 ) T_{0}(\zeta_{1})=\chi(\zeta_{1}) T 0 ( ζ 1 ) = χ ( ζ 1 ) , and there is a positive ρ 1 \rho_{1} ρ 1 with χ ( ζ ) ≤ T 0 ( ζ ) \chi(\zeta)\le T_{0}(\zeta) χ ( ζ ) ≤ T 0 ( ζ ) whenever ∥ ζ − ζ 1 ∥ < ρ 1 \lVert\zeta-\zeta_{1}\rVert<\rho_{1} ∥ ζ − ζ 1 ∥ < ρ 1 . Let ρ 0 \rho_{0} ρ 0 be positive and such that U ∗ ( ζ ) − χ ( ζ ) ≤ U ∗ ( ζ 1 ) − χ ( ζ 1 ) U^{*}(\zeta)-\chi(\zeta)\le U^{*}(\zeta_{1})-\chi(\zeta_{1}) U ∗ ( ζ ) − χ ( ζ ) ≤ U ∗ ( ζ 1 ) − χ ( ζ 1 ) for every ζ \zeta ζ with d E ( ζ , ζ 1 ) < ρ 0 d_{E}(\zeta,\zeta_{1})<\rho_{0} d E ( ζ , ζ 1 ) < ρ 0 , as the local maximum property provides. Then for every ζ \zeta ζ with ∥ ζ − ζ 1 ∥ \lVert\zeta-\zeta_{1}\rVert ∥ ζ − ζ 1 ∥ less than both ρ 0 \rho_{0} ρ 0 and ρ 1 \rho_{1} ρ 1 ,
U ∗ ( ζ ) − T 0 ( ζ ) ≤ U ∗ ( ζ ) − χ ( ζ ) ≤ U ∗ ( ζ 1 ) − χ ( ζ 1 ) = U ∗ ( ζ 1 ) − T 0 ( ζ 1 ) . U^{*}(\zeta)-T_{0}(\zeta)\ \le\ U^{*}(\zeta)-\chi(\zeta)\ \le\ U^{*}(\zeta_{1})-\chi(\zeta_{1})=U^{*}(\zeta_{1})-T_{0}(\zeta_{1}). U ∗ ( ζ ) − T 0 ( ζ ) ≤ U ∗ ( ζ ) − χ ( ζ ) ≤ U ∗ ( ζ 1 ) − χ ( ζ 1 ) = U ∗ ( ζ 1 ) − T 0 ( ζ 1 ) .
Let T = T 0 ∘ Λ T=T_{0}\circ\Lambda T = T 0 ∘ Λ . By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §quadratic , T ∈ C 2 ( H ) T\in C^{2}(H) T ∈ C 2 ( H ) , T ( x ) T(x) T ( x ) depends only on Λ x \Lambda x Λ x , the Hessian D 2 T ( x ) D^{2}T(x) D 2 T ( x ) equals the constant form
b u = ( D 2 χ ( ζ 1 ) ) Λ + 2 η 1 Π , b_{u}=\bigl(D^{2}\chi(\zeta_{1})\bigr)^{\Lambda}+2\eta_{1}\,\Pi , b u = ( D 2 χ ( ζ 1 ) ) Λ + 2 η 1 Π ,
and ∣ D T ( x ) − Λ ♯ D χ ( ζ 1 ) ∣ ≤ ( ∥ D 2 χ ( ζ 1 ) ∥ + 2 η 1 ) ∥ Λ x − ζ 1 ∥ \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 D T ( x ) − Λ ♯ Dχ ( ζ 1 ) ≤ ( ∥ D 2 χ ( ζ 1 )∥ + 2 η 1 ) ∥ Λ x − ζ 1 ∥ for every x ∈ H x\in H x ∈ 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 ,
∥ b u − X ∥ ≤ ∥ ( D 2 χ ( ζ 1 ) − X 0 ) Λ ∥ + 2 η 1 ∥ Π ∥ ≤ ε ′ + 2 η 1 . \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}. ∥ b u − X ∥ ≤ ( D 2 χ ( ζ 1 ) − X 0 ) Λ + 2 η 1 ∥ Π ∥ ≤ ε ′ + 2 η 1 .
Applying Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §majorant instead with θ \theta θ , ω 1 \omega_{1} ω 1 and the negative number − η 1 -\eta_{1} − η 1 gives a quadratic S 0 S_{0} S 0 with S 0 ( ω 1 ) = θ ( ω 1 ) S_{0}(\omega_{1})=\theta(\omega_{1}) S 0 ( ω 1 ) = θ ( ω 1 ) and a positive ρ 1 ′ \rho_{1}' ρ 1 ′ with S 0 ( ω ) ≤ θ ( ω ) S_{0}(\omega)\le\theta(\omega) S 0 ( ω ) ≤ θ ( ω ) for ∥ ω − ω 1 ∥ < ρ 1 ′ \lVert\omega-\omega_{1}\rVert<\rho_{1}' ∥ ω − ω 1 ∥ < ρ 1 ′ ; with ρ 0 ′ \rho_{0}' ρ 0 ′ a radius for the local minimum of V ∗ − θ \mathcal{V}_{*}-\theta V ∗ − θ at ω 1 \omega_{1} ω 1 , we get
V ∗ ( ω 1 ) − S 0 ( ω 1 ) ≤ V ∗ ( ω ) − S 0 ( ω ) \mathcal{V}_{*}(\omega_{1})-S_{0}(\omega_{1})\ \le\ \mathcal{V}_{*}(\omega)-S_{0}(\omega) V ∗ ( ω 1 ) − S 0 ( ω 1 ) ≤ V ∗ ( ω ) − S 0 ( ω )
whenever ∥ ω − ω 1 ∥ \lVert\omega-\omega_{1}\rVert ∥ ω − ω 1 ∥ is less than both ρ 0 ′ \rho_{0}' ρ 0 ′ and ρ 1 ′ \rho_{1}' ρ 1 ′ . Setting S = S 0 ∘ Λ S=S_{0}\circ\Lambda S = S 0 ∘ Λ , we have S ∈ C 2 ( H ) S\in C^{2}(H) S ∈ C 2 ( H ) , S ( y ) S(y) S ( y ) depends only on Λ y \Lambda y Λ y , D 2 S ( y ) D^{2}S(y) D 2 S ( y ) is the constant form b v = ( D 2 θ ( ω 1 ) ) Λ − 2 η 1 Π b_{v}=(D^{2}\theta(\omega_{1}))^{\Lambda}-2\eta_{1}\Pi b v = ( D 2 θ ( ω 1 ) ) Λ − 2 η 1 Π with ∥ b v − Y ∥ ≤ ε ′ + 2 η 1 \lVert b_{v}-Y\rVert\le\varepsilon'+2\eta_{1} ∥ b v − Y ∥ ≤ ε ′ + 2 η 1 , and ∣ D S ( y ) − Λ ♯ D θ ( ω 1 ) ∣ ≤ ( ∥ D 2 θ ( ω 1 ) ∥ + 2 η 1 ) ∥ Λ y − ω 1 ∥ \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 D S ( y ) − Λ ♯ D θ ( ω 1 ) ≤ (∥ D 2 θ ( ω 1 )∥ + 2 η 1 ) ∥ Λ y − ω 1 ∥ .
Step 5 (the fibre radius). By (iv) of Claim 3 and Real Matrices, Symmetric Matrices and the Semidefinite Ordering: Standing Notation §norm , ∥ D 2 χ ( ζ 1 ) ∥ ≤ ∥ X 0 ∥ + ε ′ ≤ 6 α + ε ′ \lVert D^{2}\chi(\zeta_{1})\rVert\le\lVert X_{0}\rVert+\varepsilon'\le6\alpha+\varepsilon' ∥ D 2 χ ( ζ 1 )∥ ≤ ∥ X 0 ∥ + ε ′ ≤ 6 α + ε ′ , and likewise for θ \theta θ ; put K = 6 α + ε ′ + 2 η 1 K=6\alpha+\varepsilon'+2\eta_{1} K = 6 α + ε ′ + 2 η 1 , so that the two gradient estimates of Step 4 hold with the factor K K K . Let r r r be a positive real number with
2 r ≤ ρ 0 , 2 r ≤ ρ 1 , 2 r ≤ ρ 0 ′ , 2 r ≤ ρ 1 ′ , r ≤ 1 , K r ≤ ε 16 , 2 ∣ α ∣ r ( D 0 + 2 ) ≤ η 0 16 , 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}, 2 r ≤ ρ 0 , 2 r ≤ ρ 1 , 2 r ≤ ρ 0 ′ , 2 r ≤ ρ 1 ′ , r ≤ 1 , Kr ≤ 16 ε , 2∣ α ∣ r ( D 0 + 2 ) ≤ 16 η 0 ,
and such that
∣ T 0 ( ζ ) − T 0 ( ζ 1 ) ∣ ≤ η 0 16 whenever ∥ ζ − ζ 1 ∥ ≤ r , ∣ S 0 ( ω ) − S 0 ( ω 1 ) ∣ ≤ η 0 16 whenever ∥ ω − ω 1 ∥ ≤ 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 . T 0 ( ζ ) − T 0 ( ζ 1 ) ≤ 16 η 0 whenever ∥ ζ − ζ 1 ∥ ≤ r , S 0 ( ω ) − S 0 ( ω 1 ) ≤ 16 η 0 whenever ∥ ω − ω 1 ∥ ≤ r .
Such an r r r exists: the first seven conditions hold for every positive r r r at most the least of the seven positive numbers
ρ 0 2 , ρ 1 2 , ρ 0 ′ 2 , ρ 1 ′ 2 , 1 , ε 16 K , η 0 16 ( 2 ∣ α ∣ ( D 0 + 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)}, 2 ρ 0 , 2 ρ 1 , 2 ρ 0 ′ , 2 ρ 1 ′ , 1 , 16 K ε , 16 ( 2∣ α ∣ ( D 0 + 2 ) + 1 ) η 0 ,
the sixth of which is defined because K K K 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 r ≤ 1 r\le1 r ≤ 1 and ( ∥ q ∥ + 1 2 ∥ M ∥ + ∣ η ∣ ) r ≤ η 0 16 (\lVert q\rVert+\tfrac12\lVert M\rVert+|\eta|)\,r\le\tfrac{\eta_{0}}{16} (∥ q ∥ + 2 1 ∥ M ∥ + ∣ η ∣ ) r ≤ 16 η 0 for each of the two quadratics, since then ∥ ζ − ζ 1 ∥ ≤ r ≤ 1 \lVert\zeta-\zeta_{1}\rVert\le r\le1 ∥ ζ − ζ 1 ∥ ≤ r ≤ 1 gives ∥ ζ − ζ 1 ∥ 2 ≤ ∥ ζ − ζ 1 ∥ ≤ r \lVert\zeta-\zeta_{1}\rVert^{2}\le\lVert\zeta-\zeta_{1}\rVert\le r ∥ ζ − ζ 1 ∥ 2 ≤ ∥ ζ − ζ 1 ∥ ≤ r . Put
A u = { x ∈ A : ∥ Λ x − ζ 1 ∥ ≤ r } , A v = { y ∈ A : ∥ Λ y − ω 1 ∥ ≤ 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\,\}. A u = { x ∈ A : ∥ Λ x − ζ 1 ∥ ≤ r } , A v = { y ∈ A : ∥ Λ y − ω 1 ∥ ≤ r } .
Step 6 (the auxiliary functions). Let Θ u , Θ v : A → R \Theta_{u},\Theta_{v}:A\to\mathbb{R} Θ u , Θ v : A → R be given by Θ u ( x ) = u ^ ( x ) − T ( x ) \Theta_{u}(x)=\hat{u}(x)-T(x) Θ u ( x ) = u ^ ( x ) − T ( x ) and Θ v ( y ) = − v ^ ( y ) + S ( y ) \Theta_{v}(y)=-\hat{v}(y)+S(y) Θ v ( y ) = − v ^ ( y ) + S ( y ) , and put
M u = U ∗ ( ζ 1 ) − T 0 ( ζ 1 ) , M v = − V ∗ ( ω 1 ) + S 0 ( ω 1 ) . M_{u}=U^{*}(\zeta_{1})-T_{0}(\zeta_{1}),\qquad M_{v}=-\mathcal{V}_{*}(\omega_{1})+S_{0}(\omega_{1}). M u = U ∗ ( ζ 1 ) − T 0 ( ζ 1 ) , M v = − V ∗ ( ω 1 ) + S 0 ( ω 1 ) .
(a) Upper bounds. Let x ∈ A u x\in A_{u} x ∈ A u . Then u ^ ( x ) ≤ U ( Λ x ) ≤ U ∗ ( Λ x ) \hat{u}(x)\le U(\Lambda x)\le U^{*}(\Lambda x) u ^ ( x ) ≤ U ( Λ x ) ≤ U ∗ ( Λ x ) , by the definition of U U U 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 ) = T 0 ( Λ x ) T(x)=T_{0}(\Lambda x) T ( x ) = T 0 ( Λ x ) with ∥ Λ x − ζ 1 ∥ ≤ r \lVert\Lambda x-\zeta_{1}\rVert\le r ∥ Λ x − ζ 1 ∥ ≤ r , which is less than both ρ 0 \rho_{0} ρ 0 and ρ 1 \rho_{1} ρ 1 . So Step 4 gives Θ u ( x ) ≤ U ∗ ( Λ x ) − T 0 ( Λ x ) ≤ M u \Theta_{u}(x)\le U^{*}(\Lambda x)-T_{0}(\Lambda x)\le M_{u} Θ u ( x ) ≤ U ∗ ( Λ x ) − T 0 ( Λ x ) ≤ M u . Symmetrically Θ v ( y ) ≤ M v \Theta_{v}(y)\le M_{v} Θ v ( y ) ≤ M v for every y ∈ A v y\in A_{v} y ∈ A v , using − v ^ ( y ) ≤ − V ( Λ y ) ≤ − V ∗ ( Λ y ) -\hat{v}(y)\le-\mathcal{V}(\Lambda y)\le-\mathcal{V}_{*}(\Lambda y) − v ^ ( y ) ≤ − V ( Λ y ) ≤ − V ∗ ( Λ y ) (claim 2 of Properties of the Lower Semicontinuous Envelope, by Duality ).
(b) Near-maximisers on a prescribed fibre neighbourhood. Let τ \tau τ and s s s be positive with s ≤ r s\le r s ≤ r . Let s ′ s' s ′ be a positive number, at most s s s , with ∣ T 0 ( ζ ) − T 0 ( ζ 1 ) ∣ ≤ τ 2 \bigl|T_{0}(\zeta)-T_{0}(\zeta_{1})\bigr|\le\tfrac{\tau}{2} T 0 ( ζ ) − T 0 ( ζ 1 ) ≤ 2 τ whenever ∥ ζ − ζ 1 ∥ ≤ s ′ \lVert\zeta-\zeta_{1}\rVert\le s' ∥ ζ − ζ 1 ∥ ≤ s ′ ; such an s ′ s' s ′ exists by the argument used for r r r in Step 5. Applying Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes §approximation with ζ 1 \zeta_{1} ζ 1 , the radius s ′ s' s ′ and the accuracy τ 2 \tfrac{\tau}{2} 2 τ gives x ∈ A x\in A x ∈ A with ∥ Λ x − ζ 1 ∥ ≤ s ′ ≤ s ≤ r \lVert\Lambda x-\zeta_{1}\rVert\le s'\le s\le r ∥ Λ x − ζ 1 ∥ ≤ s ′ ≤ s ≤ r , hence x ∈ A u x\in A_{u} x ∈ A u , and U ∗ ( ζ 1 ) − τ 2 < u ^ ( x ) U^{*}(\zeta_{1})-\tfrac{\tau}{2}<\hat{u}(x) U ∗ ( ζ 1 ) − 2 τ < u ^ ( x ) . Since T ( x ) = T 0 ( Λ x ) ≤ T 0 ( ζ 1 ) + τ 2 T(x)=T_{0}(\Lambda x)\le T_{0}(\zeta_{1})+\tfrac{\tau}{2} T ( x ) = T 0 ( Λ x ) ≤ T 0 ( ζ 1 ) + 2 τ ,
Θ u ( x ) = u ^ ( x ) − T 0 ( Λ x ) > U ∗ ( ζ 1 ) − τ 2 − T 0 ( ζ 1 ) − τ 2 = M u − 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 . Θ u ( x ) = u ^ ( x ) − T 0 ( Λ x ) > U ∗ ( ζ 1 ) − 2 τ − T 0 ( ζ 1 ) − 2 τ = M u − τ .
Applying the same clause of Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes again, this time with ω 1 \omega_{1} ω 1 in the role of ζ 1 \zeta_{1} ζ 1 , and using the second half of its conclusion (the one concerning v ^ \hat{v} v ^ and V ∗ \mathcal{V}_{*} V ∗ ) together with S 0 S_{0} S 0 in place of T 0 T_{0} T 0 , gives in the same way a y ∈ A v y\in A_{v} y ∈ A v with ∥ Λ y − ω 1 ∥ ≤ s \lVert\Lambda y-\omega_{1}\rVert\le s ∥ Λ y − ω 1 ∥ ≤ s and M v − τ < Θ v ( y ) M_{v}-\tau<\Theta_{v}(y) M v − τ < Θ v ( y ) . In particular A u A_{u} A u and A v A_{v} A v are nonempty.
(c) Closed superlevel sets. The functions g g g , k k k , T T T and S S S belong to C 2 ( H ) C^{2}(H) C 2 ( H ) : for T T T and S S S this is Step 4, and for g g g note that
g ( x ) = − α ⟨ z ˉ , x ⟩ + α ⟨ z ˉ , x ˉ ⟩ − α ( N ( x , x ) − 2 ⟨ T N x ˉ , x ⟩ + N ( x ˉ , x ˉ ) ) , 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), g ( x ) = − α ⟨ z ˉ , x ⟩ + α ⟨ z ˉ , x ˉ ⟩ − α ( N ( x , x ) − 2 ⟨ T N x ˉ , x ⟩ + N ( x ˉ , x ˉ ) ) ,
by the bilinearity and symmetry of N N N and claim 1 of The Bounded Symmetric Operator Represented by a Bounded Symmetric Bilinear Form on a Real Hilbert Space , which exhibits g g g as a sum of an affine function and a scalar multiple of x ↦ 1 2 N ( x , x ) x\mapsto\tfrac12N(x,x) x ↦ 2 1 N ( x , x ) ; so claims 1 and 2 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C 2 C^2 C 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 ∈ C 2 ( H ) g\in C^{2}(H) g ∈ C 2 ( H ) with
D g ( x ) = − α z ˉ − 2 α T N ( x − x ˉ ) , D 2 g ( x ) = − 2 α N , Dg(x)=-\alpha\bar{z}-2\alpha\,T_{N}(x-\bar{x}),\qquad D^{2}g(x)=-2\alpha N , D g ( x ) = − α z ˉ − 2 α T N ( x − x ˉ ) , D 2 g ( x ) = − 2 α N ,
and likewise k ∈ C 2 ( H ) k\in C^{2}(H) k ∈ C 2 ( H ) with D k ( y ) = α z ˉ − 2 α T N ( y − y ˉ ) Dk(y)=\alpha\bar{z}-2\alpha T_{N}(y-\bar{y}) D k ( y ) = α z ˉ − 2 α T N ( y − y ˉ ) and D 2 k ( y ) = − 2 α N D^{2}k(y)=-2\alpha N D 2 k ( y ) = − 2 α 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 , T N z = z − P z T_{N}z=z-Pz T N z = z − P z , so ∣ T N z ∣ ≤ ∣ z ∣ |T_{N}z|\le|z| ∣ T N z ∣ ≤ ∣ z ∣ .
Members of C 2 ( H ) C^{2}(H) C 2 ( H ) are differentiable on H H H and hence continuous on H H H , by The Classes C 1 C^1 C 1 and C 2 C^2 C 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 T − g T-g T − g is continuous on H H H , and Θ u ( x ) = u ( x ) − ( T ( x ) − g ( x ) ) \Theta_{u}(x)=u(x)-\bigl(T(x)-g(x)\bigr) Θ u ( x ) = u ( x ) − ( T ( x ) − g ( x ) ) , so Θ u \Theta_{u} Θ u has closed superlevel sets in H H H as a function on A A A , by claim 3 of Functions with Closed Superlevel Sets: Sequential Characterisation, Semicontinuity, Perturbation and Limits .
The restriction of Θ u \Theta_{u} Θ u to A u A_{u} A u also has closed superlevel sets in H H H . Indeed, let ( x j ) j ∈ N (x_{j})_{j\in\mathbb{N}} ( x j ) j ∈ N be a sequence in A u A_{u} A u converging to x ∈ H x\in H x ∈ H and let t ∈ R t\in\mathbb{R} t ∈ R satisfy t ≤ Θ u ( x j ) t\le\Theta_{u}(x_{j}) t ≤ Θ u ( x j ) for every j j j . By claim 1 of Functions with Closed Superlevel Sets: Sequential Characterisation, Semicontinuity, Perturbation and Limits applied to Θ u \Theta_{u} Θ u on A A A we get x ∈ A x\in A x ∈ A and t ≤ Θ u ( x ) t\le\Theta_{u}(x) t ≤ Θ u ( x ) . Moreover, for each j j j ,
∥ Λ x − ζ 1 ∥ ≤ ∥ Λ x − Λ x j ∥ + ∥ Λ x j − ζ 1 ∥ ≤ ∣ x − x j ∣ + 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 , ∥ Λ x − ζ 1 ∥ ≤ ∥ Λ x − Λ x j ∥ + ∥ Λ x j − ζ 1 ∥ ≤ ∣ x − x j ∣ + r ,
by Euclidean Distance is a Metric on R n \mathbb{R}^n R n and Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §coordinates ; since ∣ x − x j ∣ |x-x_{j}| ∣ x − x j ∣ is smaller than any prescribed positive number for suitable j j j , Comparison of Real Numbers with Arbitrary Positive Slack gives ∥ Λ x − ζ 1 ∥ ≤ r \lVert\Lambda x-\zeta_{1}\rVert\le r ∥ Λ x − ζ 1 ∥ ≤ r , so x ∈ A u x\in A_{u} x ∈ 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 H H H . The same argument applies to Θ v \Theta_{v} Θ v on A v A_{v} A v .
Step 7 (the perturbed maxima). Let λ \lambda λ be the lesser of r 8 \tfrac{r}{8} 8 r and 1 1 1 , and let μ \mu μ be a positive real with
2 μ ≤ ε 16 , 16 μ λ ≤ ε 16 , 8 μ λ 2 ≤ η 0 16 , 2\mu\le\tfrac{\varepsilon}{16},\qquad 16\mu\lambda\le\tfrac{\varepsilon}{16},\qquad 8\mu\lambda^{2}\le\tfrac{\eta_{0}}{16}, 2 μ ≤ 16 ε , 16 μ λ ≤ 16 ε , 8 μ λ 2 ≤ 16 η 0 ,
which exists as the least of three positive numbers of the required form. Then 4 λ ≤ r 2 4\lambda\le\tfrac{r}{2} 4 λ ≤ 2 r .
By (b) with τ = μ λ 2 \tau=\mu\lambda^{2} τ = μ λ 2 and s = r 4 s=\tfrac{r}{4} s = 4 r there is x 0 ∈ A u x_{0}\in A_{u} x 0 ∈ A u with ∥ Λ x 0 − ζ 1 ∥ ≤ r 4 \lVert\Lambda x_{0}-\zeta_{1}\rVert\le\tfrac{r}{4} ∥ Λ x 0 − ζ 1 ∥ ≤ 4 r and M u − μ λ 2 < Θ u ( x 0 ) M_{u}-\mu\lambda^{2}<\Theta_{u}(x_{0}) M u − μ λ 2 < Θ u ( x 0 ) . By (a), M u M_{u} M u is an upper bound for the values of Θ u \Theta_{u} Θ u on A u A_{u} A u , so the least upper bound of those values is at most Θ u ( x 0 ) + μ λ 2 \Theta_{u}(x_{0})+\mu\lambda^{2} Θ u ( x 0 ) + μ λ 2 . Hence A Perturbed Maximum Principle of Borwein-Preiss Type in a Real Hilbert Space applies to A u A_{u} A u , Θ u \Theta_{u} Θ u , μ \mu μ , λ \lambda λ and x 0 x_{0} x 0 , and provides two points, written here c 1 ∈ H c_{1}\in H c 1 ∈ H and x 1 ∈ A u x_{1}\in A_{u} x 1 ∈ A u — they are the points called y ˉ \bar{y} y ˉ and x ˉ \bar{x} x ˉ in that theorem, and are unrelated to the point y ˉ \bar{y} y ˉ of the present lemma — such that
∣ x 1 − x 0 ∣ ≤ 4 λ , ∣ x 1 − c 1 ∣ ≤ 8 λ , |x_{1}-x_{0}|\le4\lambda,\qquad |x_{1}-c_{1}|\le8\lambda, ∣ x 1 − x 0 ∣ ≤ 4 λ , ∣ x 1 − c 1 ∣ ≤ 8 λ ,
the function on A u A_{u} A u with value Θ u ( x ) − μ ∣ x − c 1 ∣ 2 \Theta_{u}(x)-\mu|x-c_{1}|^{2} Θ u ( x ) − μ ∣ x − c 1 ∣ 2 at x x x attains a sequentially strict maximum on A u A_{u} A u at x 1 x_{1} x 1 (claim 2 there), and the least upper bound of the values of Θ u \Theta_{u} Θ u on A u A_{u} A u is at most Θ u ( x 1 ) + 2 μ λ 2 \Theta_{u}(x_{1})+2\mu\lambda^{2} Θ u ( x 1 ) + 2 μ λ 2 (claim 3 there). Combining the last bound with M u − μ λ 2 < Θ u ( x 0 ) M_{u}-\mu\lambda^{2}<\Theta_{u}(x_{0}) M u − μ λ 2 < Θ u ( x 0 ) gives
M u − 3 μ λ 2 < Θ u ( x 1 ) . M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}). M u − 3 μ λ 2 < Θ u ( x 1 ) .
Also
∥ Λ x 1 − ζ 1 ∥ ≤ ∥ Λ ( x 1 − x 0 ) ∥ + ∥ Λ x 0 − ζ 1 ∥ ≤ ∣ x 1 − x 0 ∣ + r 4 ≤ 4 λ + r 4 ≤ r 2 + r 4 < 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 . ∥ Λ x 1 − ζ 1 ∥ ≤ ∥ Λ ( x 1 − x 0 )∥ + ∥ Λ x 0 − ζ 1 ∥ ≤ ∣ x 1 − x 0 ∣ + 4 r ≤ 4 λ + 4 r ≤ 2 r + 4 r < r .
The same construction on the v v v side provides c 2 ∈ H c_{2}\in H c 2 ∈ H and y 1 ∈ A v y_{1}\in A_{v} y 1 ∈ A v with ∣ y 1 − c 2 ∣ ≤ 8 λ |y_{1}-c_{2}|\le8\lambda ∣ y 1 − c 2 ∣ ≤ 8 λ , with Θ v − μ ∣ ⋅ − c 2 ∣ 2 \Theta_{v}-\mu|\cdot-c_{2}|^{2} Θ v − μ ∣ ⋅ − c 2 ∣ 2 attaining a sequentially strict maximum on A v A_{v} A v at y 1 y_{1} y 1 , with M v − 3 μ λ 2 < Θ v ( y 1 ) M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) M v − 3 μ λ 2 < Θ v ( y 1 ) and with ∥ Λ y 1 − ω 1 ∥ < r \lVert\Lambda y_{1}-\omega_{1}\rVert<r ∥ Λ y 1 − ω 1 ∥ < r .
Step 8 (the test functions and the local extrema). Define φ , ψ : H → R \varphi,\psi:H\to\mathbb{R} φ , ψ : H → R by
φ ( x ) = T ( x ) − g ( x ) + μ ∣ x − c 1 ∣ 2 , ψ ( y ) = S ( y ) + k ( y ) − μ ∣ y − c 2 ∣ 2 , \varphi(x)=T(x)-g(x)+\mu\,|x-c_{1}|^{2},
\qquad
\psi(y)=S(y)+k(y)-\mu\,|y-c_{2}|^{2}, φ ( x ) = T ( x ) − g ( x ) + μ ∣ x − c 1 ∣ 2 , ψ ( y ) = S ( y ) + k ( y ) − μ ∣ y − c 2 ∣ 2 ,
so that, for x , y ∈ A x,y\in A x , y ∈ A ,
u ( x ) − φ ( x ) = Θ u ( x ) − μ ∣ x − c 1 ∣ 2 , v ( y ) − ψ ( y ) = − ( Θ v ( y ) − μ ∣ y − c 2 ∣ 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). u ( x ) − φ ( x ) = Θ u ( x ) − μ ∣ x − c 1 ∣ 2 , v ( y ) − ψ ( y ) = − ( Θ v ( y ) − μ ∣ y − c 2 ∣ 2 ) .
Put ρ 2 = r − ∥ Λ x 1 − ζ 1 ∥ \rho_{2}=r-\lVert\Lambda x_{1}-\zeta_{1}\rVert ρ 2 = r − ∥ Λ x 1 − ζ 1 ∥ , positive by Step 7. If x ∈ A x\in A x ∈ A and ∣ x − x 1 ∣ < ρ 2 |x-x_{1}|<\rho_{2} ∣ x − x 1 ∣ < ρ 2 then
∥ Λ x − ζ 1 ∥ ≤ ∥ Λ ( x − x 1 ) ∥ + ∥ Λ x 1 − ζ 1 ∥ ≤ ∣ x − x 1 ∣ + ∥ Λ x 1 − ζ 1 ∥ < 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, ∥ Λ x − ζ 1 ∥ ≤ ∥ Λ ( x − x 1 )∥ + ∥ Λ x 1 − ζ 1 ∥ ≤ ∣ x − x 1 ∣ + ∥ Λ x 1 − ζ 1 ∥ < r ,
so x ∈ A u x\in A_{u} x ∈ A u and hence, the sequentially strict maximum of Step 7 being in particular a maximum on A u A_{u} A u (clause 1 of Sequentially Strict Maxima and Minima on a Subset of a Metric Space §maximum ),
u ( x ) − φ ( x ) = Θ u ( x ) − μ ∣ x − c 1 ∣ 2 ≤ Θ u ( x 1 ) − μ ∣ x 1 − c 1 ∣ 2 = u ( x 1 ) − φ ( x 1 ) . 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}). u ( x ) − φ ( x ) = Θ u ( x ) − μ ∣ x − c 1 ∣ 2 ≤ Θ u ( x 1 ) − μ ∣ x 1 − c 1 ∣ 2 = u ( x 1 ) − φ ( x 1 ) .
Thus u − φ u-\varphi u − φ has a local maximum at x 1 x_{1} x 1 relative to A A A . The same argument on the v v v side shows that Θ v − μ ∣ ⋅ − c 2 ∣ 2 \Theta_{v}-\mu|\cdot-c_{2}|^{2} Θ v − μ ∣ ⋅ − c 2 ∣ 2 has a local maximum at y 1 y_{1} y 1 relative to A A A , hence that v − ψ v-\psi v − ψ , being its additive inverse there, has a local minimum at y 1 y_{1} y 1 relative to A A A .
By Step 4, Step 6(c) and claim 3 of Affine and Quadratic Functions on a Real Hilbert Space are of Class C 2 C^2 C 2 (applied with 2 μ 2\mu 2 μ in the role of the coefficient), each of T T T , g g g , S S S , k k k and the two squared-distance terms belongs to C 2 ( H ) C^{2}(H) C 2 ( H ) ; so φ , ψ ∈ C 2 ( H ) \varphi,\psi\in C^{2}(H) φ , ψ ∈ 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
D φ ( x 1 ) = D T ( x 1 ) − D g ( x 1 ) + 2 μ ( x 1 − c 1 ) , D 2 φ ( x 1 ) = b u + 2 α N + 2 μ I , 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, D φ ( x 1 ) = D T ( x 1 ) − D g ( x 1 ) + 2 μ ( x 1 − c 1 ) , D 2 φ ( x 1 ) = b u + 2 α N + 2 μ I ,
D ψ ( y 1 ) = D S ( y 1 ) + D k ( y 1 ) − 2 μ ( y 1 − c 2 ) , D 2 ψ ( y 1 ) = b v − 2 α N − 2 μ I . 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 . D ψ ( y 1 ) = D S ( y 1 ) + D k ( y 1 ) − 2 μ ( y 1 − c 2 ) , D 2 ψ ( y 1 ) = b v − 2 α N − 2 μ I .
Step 9 (the localisation). Write Ξ ( x , y ) = u ^ ( x ) − v ^ ( y ) − α 2 ∥ Λ x − Λ y ∥ 2 \Xi(x,y)=\hat{u}(x)-\hat{v}(y)-\tfrac{\alpha}{2}\lVert\Lambda x-\Lambda y\rVert^{2} Ξ ( x , y ) = u ^ ( x ) − v ^ ( y ) − 2 α ∥ Λ x − Λ y ∥ 2 for x , y ∈ A x,y\in A x , y ∈ A , and M 1 = Ξ ( x ˉ , y ˉ ) M_{1}=\Xi(\bar{x},\bar{y}) M 1 = Ξ ( x ˉ , y ˉ ) ; by Claim 2, Φ ( x , y ) ≥ Ξ ( x , y ) − α 2 ∣ z ˉ ∣ 2 \Phi(x,y)\ge\Xi(x,y)-\tfrac{\alpha}{2}|\bar{z}|^{2} Φ ( x , y ) ≥ Ξ ( x , y ) − 2 α ∣ z ˉ ∣ 2 and M 1 = M 0 + α 2 ∣ z ˉ ∣ 2 M_{1}=M_{0}+\tfrac{\alpha}{2}|\bar{z}|^{2} M 1 = M 0 + 2 α ∣ z ˉ ∣ 2 . Since T ( x 1 ) = T 0 ( Λ x 1 ) T(x_{1})=T_{0}(\Lambda x_{1}) T ( x 1 ) = T 0 ( Λ x 1 ) and S ( y 1 ) = S 0 ( Λ y 1 ) S(y_{1})=S_{0}(\Lambda y_{1}) S ( y 1 ) = S 0 ( Λ y 1 ) ,
Ξ ( x 1 , y 1 ) = Θ u ( x 1 ) + Θ v ( y 1 ) + T 0 ( Λ x 1 ) − S 0 ( Λ y 1 ) − α 2 ∥ Λ x 1 − Λ y 1 ∥ 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}. Ξ ( x 1 , y 1 ) = Θ u ( x 1 ) + Θ v ( y 1 ) + T 0 ( Λ x 1 ) − S 0 ( Λ y 1 ) − 2 α ∥ Λ x 1 − Λ y 1 ∥ 2 .
By Step 3 and Fibre Suprema along a Coordinate Map and Their Semicontinuous Envelopes §values (through Claim 3),
M u + M v = U ∗ ( ζ 1 ) − V ∗ ( ω 1 ) − T 0 ( ζ 1 ) + S 0 ( ω 1 ) > U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) − 2 ε ′ − T 0 ( ζ 1 ) + S 0 ( ω 1 ) , 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}), M u + M v = U ∗ ( ζ 1 ) − V ∗ ( ω 1 ) − T 0 ( ζ 1 ) + S 0 ( ω 1 ) > U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) − 2 ε ′ − T 0 ( ζ 1 ) + S 0 ( ω 1 ) ,
and U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) = u ^ ( x ˉ ) − v ^ ( y ˉ ) = M 1 + α 2 D 0 2 U^{*}(\bar{\zeta})-\mathcal{V}_{*}(\bar{\omega})=\hat{u}(\bar{x})-\hat{v}(\bar{y})=M_{1}+\tfrac{\alpha}{2}D_{0}^{2} U ∗ ( ζ ˉ ) − V ∗ ( ω ˉ ) = u ^ ( x ˉ ) − v ^ ( y ˉ ) = M 1 + 2 α D 0 2 . With M u − 3 μ λ 2 < Θ u ( x 1 ) M_{u}-3\mu\lambda^{2}<\Theta_{u}(x_{1}) M u − 3 μ λ 2 < Θ u ( x 1 ) and M v − 3 μ λ 2 < Θ v ( y 1 ) M_{v}-3\mu\lambda^{2}<\Theta_{v}(y_{1}) M v − 3 μ λ 2 < Θ v ( y 1 ) from Step 7, this gives
Ξ ( x 1 , y 1 ) > M 1 + α 2 D 0 2 − 2 ε ′ − 6 μ λ 2 + [ T 0 ( Λ x 1 ) − T 0 ( ζ 1 ) ] − [ S 0 ( Λ y 1 ) − S 0 ( ω 1 ) ] − α 2 ∥ Λ x 1 − Λ y 1 ∥ 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}. Ξ ( x 1 , y 1 ) > M 1 + 2 α D 0 2 − 2 ε ′ − 6 μ λ 2 + [ T 0 ( Λ x 1 ) − T 0 ( ζ 1 ) ] − [ S 0 ( Λ y 1 ) − S 0 ( ω 1 ) ] − 2 α ∥ Λ x 1 − Λ y 1 ∥ 2 .
By Step 7 we have ∥ Λ x 1 − ζ 1 ∥ ≤ r \lVert\Lambda x_{1}-\zeta_{1}\rVert\le r ∥ Λ x 1 − ζ 1 ∥ ≤ r and ∥ Λ y 1 − ω 1 ∥ ≤ r \lVert\Lambda y_{1}-\omega_{1}\rVert\le r ∥ Λ y 1 − ω 1 ∥ ≤ r , so each of the two bracketed terms has absolute value at most η 0 16 \tfrac{\eta_{0}}{16} 16 η 0 by Step 5, and therefore each is at least − η 0 16 -\tfrac{\eta_{0}}{16} − 16 η 0 by claim 3 of Properties of the Absolute Value in an Ordered Field . Next, ∥ ζ ˉ − Λ x 1 ∥ ≤ ∥ ζ ˉ − ζ 1 ∥ + ∥ ζ 1 − Λ x 1 ∥ < 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 ∥ ζ ˉ − Λ x 1 ∥ ≤ ∥ ζ ˉ − ζ 1 ∥ + ∥ ζ 1 − Λ x 1 ∥ < ε ′ + r and similarly ∥ ω ˉ − Λ y 1 ∥ < ε ′ + r \lVert\bar{\omega}-\Lambda y_{1}\rVert<\varepsilon'+r ∥ ω ˉ − Λ y 1 ∥ < ε ′ + r ; so Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §stability , applied with ( ζ ˉ , ω ˉ ) (\bar{\zeta},\bar{\omega}) ( ζ ˉ , ω ˉ ) and ( Λ x 1 , Λ y 1 ) (\Lambda x_{1},\Lambda y_{1}) ( Λ x 1 , Λ y 1 ) , gives ∥ Λ x 1 − Λ y 1 ∥ ≤ D 0 + 2 ( ε ′ + r ) ≤ D 0 + 4 \lVert\Lambda x_{1}-\Lambda y_{1}\rVert\le D_{0}+2(\varepsilon'+r)\le D_{0}+4 ∥ Λ x 1 − Λ y 1 ∥ ≤ D 0 + 2 ( ε ′ + r ) ≤ D 0 + 4 (as ε ′ ≤ 1 \varepsilon'\le1 ε ′ ≤ 1 and r ≤ 1 r\le1 r ≤ 1 ) and hence
∣ α 2 D 0 2 − α 2 ∥ Λ x 1 − Λ y 1 ∥ 2 ∣ ≤ ∣ α ∣ 2 ( 2 D 0 + 4 ) ⋅ 2 ( ε ′ + r ) = 2 ∣ α ∣ ( ε ′ + r ) ( D 0 + 2 ) ≤ η 0 16 + η 0 16 , \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}, 2 α D 0 2 − 2 α ∥ Λ x 1 − Λ y 1 ∥ 2 ≤ 2 ∣ α ∣ ( 2 D 0 + 4 ) ⋅ 2 ( ε ′ + r ) = 2∣ α ∣ ( ε ′ + r ) ( D 0 + 2 ) ≤ 16 η 0 + 16 η 0 ,
by Steps 2 and 5. Since also 2 ε ′ ≤ η 0 8 2\varepsilon'\le\tfrac{\eta_{0}}{8} 2 ε ′ ≤ 8 η 0 and 6 μ λ 2 ≤ η 0 16 6\mu\lambda^{2}\le\tfrac{\eta_{0}}{16} 6 μ λ 2 ≤ 16 η 0 , we conclude
Ξ ( x 1 , y 1 ) > M 1 − η 0 8 − η 0 16 − η 0 16 − η 0 16 − η 0 16 − η 0 16 ≥ M 1 − η 0 , \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}, Ξ ( x 1 , y 1 ) > M 1 − 8 η 0 − 16 η 0 − 16 η 0 − 16 η 0 − 16 η 0 − 16 η 0 ≥ M 1 − η 0 ,
and therefore Φ ( x 1 , y 1 ) ≥ Ξ ( x 1 , y 1 ) − α 2 ∣ z ˉ ∣ 2 > M 1 − η 0 − α 2 ∣ z ˉ ∣ 2 = M 0 − η 0 \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} Φ ( x 1 , y 1 ) ≥ Ξ ( x 1 , y 1 ) − 2 α ∣ z ˉ ∣ 2 > M 1 − η 0 − 2 α ∣ z ˉ ∣ 2 = M 0 − η 0 . By Step 1,
∣ x 1 − x ˉ ∣ < ε 1 ≤ ε , ∣ y 1 − y ˉ ∣ < ε 1 ≤ ε , ∣ u ( x 1 ) − u ( x ˉ ) ∣ < ε 1 ≤ ε , ∣ v ( y 1 ) − v ( y ˉ ) ∣ < ε 1 ≤ 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, ∣ x 1 − x ˉ ∣ < ε 1 ≤ ε , ∣ y 1 − y ˉ ∣ < ε 1 ≤ ε , ∣ u ( x 1 ) − u ( x ˉ ) ∣ < ε 1 ≤ ε , ∣ v ( y 1 ) − v ( y ˉ ) ∣ < ε 1 ≤ ε ,
which are four of the eight required inequalities.
Step 10 (the gradients and Hessians). By Step 8, Step 6(c) and Claim 3,
D φ ( x 1 ) − p = ( D T ( x 1 ) − Λ ♯ D χ ( ζ 1 ) ) + Λ ♯ ( D χ ( ζ 1 ) − p 0 ) + 2 α T N ( x 1 − x ˉ ) + 2 μ ( x 1 − c 1 ) , 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}), D φ ( x 1 ) − p = ( D T ( x 1 ) − Λ ♯ Dχ ( ζ 1 ) ) + Λ ♯ ( Dχ ( ζ 1 ) − p 0 ) + 2 α T N ( x 1 − x ˉ ) + 2 μ ( x 1 − c 1 ) ,
because − D g ( x 1 ) = α z ˉ + 2 α T N ( x 1 − x ˉ ) -Dg(x_{1})=\alpha\bar{z}+2\alpha T_{N}(x_{1}-\bar{x}) − D g ( x 1 ) = α z ˉ + 2 α T N ( x 1 − x ˉ ) , because Λ ♯ \Lambda^{\sharp} Λ ♯ is linear, and because p = Λ ♯ p 0 + α z ˉ p=\Lambda^{\sharp}p_{0}+\alpha\bar{z} p = Λ ♯ p 0 + α z ˉ . The four terms are estimated in turn: the first has norm at most K ∥ Λ x 1 − ζ 1 ∥ ≤ K r ≤ ε 16 K\lVert\Lambda x_{1}-\zeta_{1}\rVert\le Kr\le\tfrac{\varepsilon}{16} K ∥ Λ x 1 − ζ 1 ∥ ≤ Kr ≤ 16 ε by Steps 4, 5 and 7; the second has norm ∥ D χ ( ζ 1 ) − p 0 ∥ < ε ′ ≤ ε 16 \lVert D\chi(\zeta_{1})-p_{0}\rVert<\varepsilon'\le\tfrac{\varepsilon}{16} ∥ Dχ ( ζ 1 ) − p 0 ∥ < ε ′ ≤ 16 ε , since ∣ Λ ♯ ξ ∣ = ∥ ξ ∥ |\Lambda^{\sharp}\xi|=\lVert\xi\rVert ∣ Λ ♯ ξ ∣ = ∥ ξ ∥ ; the third has norm at most 2 α ∣ x 1 − x ˉ ∣ < 2 α ε 1 ≤ ε 4 2\alpha|x_{1}-\bar{x}|<2\alpha\varepsilon_{1}\le\tfrac{\varepsilon}{4} 2 α ∣ x 1 − x ˉ ∣ < 2 α ε 1 ≤ 4 ε by ∣ T N z ∣ ≤ ∣ z ∣ |T_{N}z|\le|z| ∣ T N z ∣ ≤ ∣ z ∣ , Step 9 and ε 1 ≤ ε 8 α \varepsilon_{1}\le\tfrac{\varepsilon}{8\alpha} ε 1 ≤ 8 α ε ; and the fourth has norm 2 μ ∣ x 1 − c 1 ∣ ≤ 16 μ λ ≤ ε 16 2\mu|x_{1}-c_{1}|\le16\mu\lambda\le\tfrac{\varepsilon}{16} 2 μ ∣ x 1 − c 1 ∣ ≤ 16 μ λ ≤ 16 ε by Step 7. By the triangle inequality (claim 1 of The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity ),
∣ D φ ( x 1 ) − p ∣ ≤ ε 16 + ε 16 + ε 4 + ε 16 < ε . \bigl|D\varphi(x_{1})-p\bigr|\le\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{16}+\tfrac{\varepsilon}{4}+\tfrac{\varepsilon}{16}<\varepsilon . D φ ( x 1 ) − p ≤ 16 ε + 16 ε + 4 ε + 16 ε < ε .
For the Hessian, D 2 φ ( x 1 ) − ( X + 2 α N ) = ( b u − X ) + 2 μ I D^{2}\varphi(x_{1})-(X+2\alpha N)=(b_{u}-X)+2\mu I D 2 φ ( x 1 ) − ( X + 2 α N ) = ( b u − X ) + 2 μ 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,
∥ D 2 φ ( x 1 ) − ( X + 2 α N ) ∥ ≤ ∥ b u − X ∥ + 2 μ ∥ I ∥ ≤ ( ε ′ + 2 η 1 ) + 2 μ ≤ ε 16 + ε 16 + ε 16 < 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 . D 2 φ ( x 1 ) − ( X + 2 α N ) ≤ ∥ b u − X ∥ + 2 μ ∥ I ∥ ≤ ( ε ′ + 2 η 1 ) + 2 μ ≤ 16 ε + 16 ε + 16 ε < ε .
On the v v v side, D k ( y 1 ) = α z ˉ − 2 α T N ( y 1 − y ˉ ) Dk(y_{1})=\alpha\bar{z}-2\alpha T_{N}(y_{1}-\bar{y}) D k ( y 1 ) = α z ˉ − 2 α T N ( y 1 − y ˉ ) , so
D ψ ( y 1 ) − p = ( D S ( y 1 ) − Λ ♯ D θ ( ω 1 ) ) + Λ ♯ ( D θ ( ω 1 ) − p 0 ) − 2 α T N ( y 1 − y ˉ ) − 2 μ ( y 1 − c 2 ) , 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}), D ψ ( y 1 ) − p = ( D S ( y 1 ) − Λ ♯ D θ ( ω 1 ) ) + Λ ♯ ( D θ ( ω 1 ) − p 0 ) − 2 α T N ( y 1 − y ˉ ) − 2 μ ( y 1 − c 2 ) ,
and the same four estimates, with ∥ Λ y 1 − ω 1 ∥ ≤ r \lVert\Lambda y_{1}-\omega_{1}\rVert\le r ∥ Λ y 1 − ω 1 ∥ ≤ r and ∣ y 1 − y ˉ ∣ < ε 1 |y_{1}-\bar{y}|<\varepsilon_{1} ∣ y 1 − y ˉ ∣ < ε 1 in place of their counterparts, give ∣ D ψ ( y 1 ) − p ∣ < ε |D\psi(y_{1})-p|<\varepsilon ∣ D ψ ( y 1 ) − p ∣ < ε . Finally D 2 ψ ( y 1 ) − ( Y − 2 α N ) = ( b v − Y ) − 2 μ I D^{2}\psi(y_{1})-(Y-2\alpha N)=(b_{v}-Y)-2\mu I D 2 ψ ( y 1 ) − ( Y − 2 α N ) = ( b v − Y ) − 2 μ I , whose norm is at most ( ε ′ + 2 η 1 ) + 2 μ < ε (\varepsilon'+2\eta_{1})+2\mu<\varepsilon ( ε ′ + 2 η 1 ) + 2 μ < ε as before.
This establishes all eight inequalities and completes the proof of Claim 4, hence of clause 1 and of the lemma.