Each result cited is universally quantified over the data in its own statement. Throughout, x , y ∈ D ( A ) x,y\in D(A) x , y ∈ D ( A ) , and we write a = A x a=Ax a = A x , b = A y b=Ay b = A y and Φ ( z ) = B ( z ) + L ( z ) \Phi(z)=B(z)+L(z) Φ ( z ) = B ( z ) + L ( z ) for z ∈ V z\in V z ∈ V ; norms and pairings without a subscript are those of H H H . By The Penalty Function h = 1 2 ∣ ⋅ ∣ V 2 h=\tfrac12|\cdot|_V^2 h = 2 1 ∣ ⋅ ∣ V 2 of a Hilbert Triple: Expansion Identities, Closed Sublevel Sets, Density and Local Bounds §nonneg we have 0 ≤ h ( z ) 0\le h(z) 0 ≤ h ( z ) for z ∈ V z\in V z ∈ V , and 2 h ( z ) = ∣ z ∣ V 2 2h(z)=|z|_{V}^{2} 2 h ( z ) = ∣ z ∣ V 2 by Hilbert Triples: Standing Notation and Background §penalty . By Hilbert Triples: Standing Notation and Background §triple we have ∣ z ∣ H ≤ ∣ z ∣ V |z|_{H}\le|z|_{V} ∣ z ∣ H ≤ ∣ z ∣ V for z ∈ V z\in V z ∈ V . By Elementary Properties of a Hilbert Triple: the Embedding, the Riesz Map and the Form Operator §symmetric , ⟨ A z , v ⟩ H = ⟨ z , v ⟩ V \langle Az,v\rangle_{H}=\langle z,v\rangle_{V} ⟨ A z , v ⟩ H = ⟨ z , v ⟩ V for z ∈ D ( A ) z\in D(A) z ∈ D ( A ) and v ∈ V v\in V v ∈ V .
Since L L L is Lipschitz with constant ℓ \ell ℓ , ∣ L ( z ) − L ( v ) ∣ ≤ ℓ ∣ z − v ∣ |L(z)-L(v)|\le\ell|z-v| ∣ L ( z ) − L ( v ) ∣ ≤ ℓ ∣ z − v ∣ for z , v ∈ H z,v\in H z , v ∈ H , and taking v = 0 H v=0_{H} v = 0 H and using The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle gives
∣ L ( z ) ∣ ≤ c L + ℓ ∣ z ∣ for every z ∈ H . |L(z)|\le c_{L}+\ell|z|\qquad\text{for every }z\in H . ∣ L ( z ) ∣ ≤ c L + ℓ ∣ z ∣ for every z ∈ H .
We use the following three elementary facts. First, by Elementary Identities in a Real Inner Product Space §expansion , 1 2 ∣ c ∣ 2 + ⟨ u , c ⟩ = 1 2 ∣ c + u ∣ 2 − 1 2 ∣ u ∣ 2 \tfrac{1}{2}|c|^{2}+\langle u,c\rangle=\tfrac{1}{2}|c+u|^{2}-\tfrac{1}{2}|u|^{2} 2 1 ∣ c ∣ 2 + ⟨ u , c ⟩ = 2 1 ∣ c + u ∣ 2 − 2 1 ∣ u ∣ 2 for u , c ∈ H u,c\in H u , c ∈ H . Secondly, for real c > 0 c>0 c > 0 and u , v u,v u , v with 0 ≤ u 0\le u 0 ≤ u and 0 ≤ v 0\le v 0 ≤ v , expanding 0 ≤ 1 c ( c u − v ) 2 0\le\tfrac{1}{c}(c\,u-v)^{2} 0 ≤ c 1 ( c u − v ) 2 gives 2 u v ≤ c u 2 + v 2 c 2uv\le c\,u^{2}+\tfrac{v^{2}}{c} 2 uv ≤ c u 2 + c v 2 ; we use it as u v ≤ 1 4 u 2 + v 2 uv\le\tfrac{1}{4}u^{2}+v^{2} uv ≤ 4 1 u 2 + v 2 (the case c = 1 2 c=\tfrac{1}{2} c = 2 1 ) and in the displayed forms below. Thirdly, ( s + t ) 2 ≤ 2 s 2 + 2 t 2 (s+t)^{2}\le2s^{2}+2t^{2} ( s + t ) 2 ≤ 2 s 2 + 2 t 2 for real s , t s,t s , t , by Products and Sums of Weighted Square-Summable Sequences of Real Numbers §pointwise .
Claim 1. The values of F F F are real numbers and its domain is D ( A ) × R × H × S y m ( V ) D(A)\times\mathbb{R}\times H\times\mathrm{Sym}(V) D ( A ) × R × H × Sym ( V ) , which with W = D ( A ) W=D(A) W = D ( A ) is what Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ \delta δ -Shifts §operator requires of a second-order equation operator on H H H . The defining expression does not contain its fourth argument, so F ( x , r , p , X ) = F ( x , r , p , X ′ ) F(x,r,p,X)=F(x,r,p,X') F ( x , r , p , X ) = F ( x , r , p , X ′ ) for all X , X ′ ∈ S y m ( V ) X,X'\in\mathrm{Sym}(V) X , X ′ ∈ Sym ( V ) , which is First-Order Equation Operator on a Hilbert Triple §first-order . Degenerate ellipticity is then A First-Order Equation Operator is Degenerate Elliptic and Its δ \delta δ -Shifts Ignore the Form Argument §elliptic .
Claim 2. Let R R R be positive, x ∈ D ( A ) x\in D(A) x ∈ D ( A ) , p ∈ H p\in H p ∈ H , X ∈ S y m ( V ) X\in\mathrm{Sym}(V) X ∈ Sym ( V ) and r , s ∈ R r,s\in\mathbb{R} r , s ∈ R with − R ≤ s ≤ r ≤ R -R\le s\le r\le R − R ≤ s ≤ r ≤ R . Every term of F F F other than λ 0 r \lambda_{0}r λ 0 r is independent of the second argument, so
F ( x , r , p , X ) − F ( x , s , p , X ) = λ 0 r − λ 0 s = λ 0 ( r − s ) , F(x,r,p,X)-F(x,s,p,X)=\lambda_{0}r-\lambda_{0}s=\lambda_{0}(r-s), F ( x , r , p , X ) − F ( x , s , p , X ) = λ 0 r − λ 0 s = λ 0 ( r − s ) ,
and in particular λ 0 ( r − s ) ≤ F ( x , r , p , X ) − F ( x , s , p , X ) \lambda_{0}(r-s)\le F(x,r,p,X)-F(x,s,p,X) λ 0 ( r − s ) ≤ F ( x , r , p , X ) − F ( x , s , p , X ) . As λ 0 \lambda_{0} λ 0 is positive, this is the requirement of Locally Strictly Proper Second-Order Equation Operator on a Hilbert Triple §constant ; since R R R was an arbitrary positive real, F F F is locally strictly proper by Locally Strictly Proper Second-Order Equation Operator on a Hilbert Triple §strictly-proper .
The shifts. Let δ ∈ R \delta\in\mathbb{R} δ ∈ R satisfy 0 < δ < 1 0<\delta<1 0 < δ < 1 . By Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ \delta δ -Shifts §shifted and claim 1, the δ \delta δ -shifts do not depend on their fourth argument and are given by
F δ − ( x , r , p , X ) = λ 0 ( r + δ h ( x ) ) + 1 2 ∣ p + δ a ∣ 2 + ⟨ a + Φ ( x ) , p + δ a ⟩ − g ( x ) , F^{-}_{\delta}(x,r,p,X)=\lambda_{0}\bigl(r+\delta h(x)\bigr)+\tfrac{1}{2}|p+\delta a|^{2}+\langle a+\Phi(x),p+\delta a\rangle-g(x), F δ − ( x , r , p , X ) = λ 0 ( r + δ h ( x ) ) + 2 1 ∣ p + δ a ∣ 2 + ⟨ a + Φ ( x ) , p + δ a ⟩ − g ( x ) ,
F δ + ( y , s , p ′ , X ′ ) = λ 0 ( s − δ h ( y ) ) + 1 2 ∣ p ′ − δ b ∣ 2 + ⟨ b + Φ ( y ) , p ′ − δ b ⟩ − g ( y ) . F^{+}_{\delta}(y,s,p',X')=\lambda_{0}\bigl(s-\delta h(y)\bigr)+\tfrac{1}{2}|p'-\delta b|^{2}+\langle b+\Phi(y),p'-\delta b\rangle-g(y). F δ + ( y , s , p ′ , X ′ ) = λ 0 ( s − δ h ( y ) ) + 2 1 ∣ p ′ − δ b ∣ 2 + ⟨ b + Φ ( y ) , p ′ − δ b ⟩ − g ( y ) .
By the first elementary fact, with c = p + δ a c=p+\delta a c = p + δ a and u = a u=a u = a , and with c = p ′ − δ b c=p'-\delta b c = p ′ − δ b and u = b u=b u = b ,
F δ − ( x , r , p , X ) = λ 0 ( r + δ h ( x ) ) + 1 2 ∣ p + ( 1 + δ ) a ∣ 2 − 1 2 ∣ a ∣ 2 + ⟨ Φ ( x ) , p + δ a ⟩ − g ( x ) , ( ∗ ) F^{-}_{\delta}(x,r,p,X)=\lambda_{0}\bigl(r+\delta h(x)\bigr)+\tfrac{1}{2}\bigl|p+(1+\delta)a\bigr|^{2}-\tfrac{1}{2}|a|^{2}+\langle\Phi(x),p+\delta a\rangle-g(x),\tag{$*$} F δ − ( x , r , p , X ) = λ 0 ( r + δ h ( x ) ) + 2 1 p + ( 1 + δ ) a 2 − 2 1 ∣ a ∣ 2 + ⟨ Φ ( x ) , p + δ a ⟩ − g ( x ) , ( ∗ )
F δ + ( y , s , p ′ , X ′ ) = λ 0 ( s − δ h ( y ) ) + 1 2 ∣ p ′ + ( 1 − δ ) b ∣ 2 − 1 2 ∣ b ∣ 2 + ⟨ Φ ( y ) , p ′ − δ b ⟩ − g ( y ) . ( ∗ ∗ ) F^{+}_{\delta}(y,s,p',X')=\lambda_{0}\bigl(s-\delta h(y)\bigr)+\tfrac{1}{2}\bigl|p'+(1-\delta)b\bigr|^{2}-\tfrac{1}{2}|b|^{2}+\langle\Phi(y),p'-\delta b\rangle-g(y).\tag{$**$} F δ + ( y , s , p ′ , X ′ ) = λ 0 ( s − δ h ( y ) ) + 2 1 p ′ + ( 1 − δ ) b 2 − 2 1 ∣ b ∣ 2 + ⟨ Φ ( y ) , p ′ − δ b ⟩ − g ( y ) . ( ∗ ∗ )
Claim 3, the two moduli. By The Nondecreasing Envelope of a Truncated Modulus of Continuity §modulus the function ω ˉ g \bar{\omega}_{g} ω ˉ g is a modulus of continuity satisfying 0 ≤ ω ˉ g ( t ) ≤ 2 C g 0\le\bar{\omega}_{g}(t)\le2C_{g} 0 ≤ ω ˉ g ( t ) ≤ 2 C g for every nonnegative t t t ; as 2 C g 2C_{g} 2 C g is nonnegative, its quadratic reparametrisation ω g ∗ \omega_{g}^{\ast} ω g ∗ at 2 C g 2C_{g} 2 C g is therefore defined, and is a nondecreasing modulus of continuity, by Sums, Nonnegative Multiples, Monotonicity and Quadratic Reparametrisation of Moduli of Continuity §quadratic . By Linear Moduli of Continuity §modulus the function t ↦ ℓ t t\mapsto\ell t t ↦ ℓ t is a modulus of continuity, since 0 ≤ ℓ 0\le\ell 0 ≤ ℓ ; so ω 1 \omega_{1} ω 1 is a modulus of continuity by Sums, Nonnegative Multiples, Monotonicity and Quadratic Reparametrisation of Moduli of Continuity §sum . For a real α > 1 \alpha>1 α > 1 the number K α K\alpha K α is nonnegative, being a product of positive numbers, so t ↦ K α t t\mapsto K\alpha t t ↦ K α t is a modulus of continuity by Linear Moduli of Continuity §modulus .
Claim 3, the inequality. Let R R R be positive, let x , y ∈ D ( A ) x,y\in D(A) x , y ∈ D ( A ) , let r ∈ R r\in\mathbb{R} r ∈ R with − R ≤ r ≤ R -R\le r\le R − R ≤ r ≤ R , let X , Y ∈ S y m ( H ) X,Y\in\mathrm{Sym}(H) X , Y ∈ Sym ( H ) and let α , δ ∈ R \alpha,\delta\in\mathbb{R} α , δ ∈ R with 1 < α 1<\alpha 1 < α and 0 < δ < 1 0<\delta<1 0 < δ < 1 . Put w = α ( x − y ) w=\alpha(x-y) w = α ( x − y ) and σ = α ∣ x − y ∣ 2 + 1 α \sigma=\alpha|x-y|^{2}+\tfrac{1}{\alpha} σ = α ∣ x − y ∣ 2 + α 1 , and let D = F δ − ( x , r , w , X ) − F δ + ( y , r , w , Y ) D=F^{-}_{\delta}(x,r,w,X)-F^{+}_{\delta}(y,r,w,Y) D = F δ − ( x , r , w , X ) − F δ + ( y , r , w , Y ) . Expanding the two shift formulas and Elementary Identities in a Real Inner Product Space §expansion ,
D = λ 0 δ ( h ( x ) + h ( y ) ) + δ ⟨ w , a + b ⟩ + δ 2 2 ( ∣ a ∣ 2 − ∣ b ∣ 2 ) + ⟨ a − b , w ⟩ + ⟨ Φ ( x ) − Φ ( y ) , w ⟩ + δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) + δ ( ⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩ ) − ( g ( x ) − g ( y ) ) . D=\lambda_{0}\delta\bigl(h(x)+h(y)\bigr)+\delta\langle w,a+b\rangle+\tfrac{\delta^{2}}{2}\bigl(|a|^{2}-|b|^{2}\bigr)+\langle a-b,w\rangle+\langle\Phi(x)-\Phi(y),w\rangle+\delta\bigl(|a|^{2}+|b|^{2}\bigr)+\delta\bigl(\langle\Phi(x),a\rangle+\langle\Phi(y),b\rangle\bigr)-\bigl(g(x)-g(y)\bigr). D = λ 0 δ ( h ( x ) + h ( y ) ) + δ ⟨ w , a + b ⟩ + 2 δ 2 ( ∣ a ∣ 2 − ∣ b ∣ 2 ) + ⟨ a − b , w ⟩ + ⟨ Φ ( x ) − Φ ( y ) , w ⟩ + δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) + δ ( ⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩ ) − ( g ( x ) − g ( y ) ) .
We bound the eight groups in turn, taking the fourth and the eighth together in (vii) .
(i) 0 ≤ λ 0 δ ( h ( x ) + h ( y ) ) 0\le\lambda_{0}\delta(h(x)+h(y)) 0 ≤ λ 0 δ ( h ( x ) + h ( y )) , all three factors being nonnegative.
(ii) Since x − y ∈ V x-y\in V x − y ∈ V , the symmetry identity gives ⟨ a − b , w ⟩ = α ( ⟨ x , x − y ⟩ V − ⟨ y , x − y ⟩ V ) = α ∣ x − y ∣ V 2 \langle a-b,w\rangle=\alpha\bigl(\langle x,x-y\rangle_{V}-\langle y,x-y\rangle_{V}\bigr)=\alpha|x-y|_{V}^{2} ⟨ a − b , w ⟩ = α ( ⟨ x , x − y ⟩ V − ⟨ y , x − y ⟩ V ) = α ∣ x − y ∣ V 2 , which is nonnegative. This term is not discarded: it is combined with the eighth group in (vii) , where it absorbs the oscillation of g g g .
(iii) Likewise ⟨ w , a + b ⟩ = α ( ⟨ x , x − y ⟩ V + ⟨ y , x − y ⟩ V ) = α ( ∣ x ∣ V 2 − ∣ y ∣ V 2 ) = 2 α ( h ( x ) − h ( y ) ) \langle w,a+b\rangle=\alpha\bigl(\langle x,x-y\rangle_{V}+\langle y,x-y\rangle_{V}\bigr)=\alpha\bigl(|x|_{V}^{2}-|y|_{V}^{2}\bigr)=2\alpha\bigl(h(x)-h(y)\bigr) ⟨ w , a + b ⟩ = α ( ⟨ x , x − y ⟩ V + ⟨ y , x − y ⟩ V ) = α ( ∣ x ∣ V 2 − ∣ y ∣ V 2 ) = 2 α ( h ( x ) − h ( y ) ) , so, h h h being nonnegative,
δ ⟨ w , a + b ⟩ ≥ − 2 α δ h ( y ) ≥ − 2 α ⋅ δ ( h ( x ) + h ( y ) + 1 ) . \delta\langle w,a+b\rangle\ge-2\alpha\,\delta\,h(y)\ge-2\alpha\cdot\delta\bigl(h(x)+h(y)+1\bigr). δ ⟨ w , a + b ⟩ ≥ − 2 α δ h ( y ) ≥ − 2 α ⋅ δ ( h ( x ) + h ( y ) + 1 ) .
(iv) Since 0 < δ < 1 0<\delta<1 0 < δ < 1 we have 1 2 ≤ 1 − δ 2 \tfrac{1}{2}\le1-\tfrac{\delta}{2} 2 1 ≤ 1 − 2 δ and 1 2 ≤ 1 + δ 2 \tfrac{1}{2}\le1+\tfrac{\delta}{2} 2 1 ≤ 1 + 2 δ , so
δ 2 2 ( ∣ a ∣ 2 − ∣ b ∣ 2 ) + δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) = δ ( 1 + δ 2 ) ∣ a ∣ 2 + δ ( 1 − δ 2 ) ∣ b ∣ 2 ≥ δ 2 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) . \tfrac{\delta^{2}}{2}\bigl(|a|^{2}-|b|^{2}\bigr)+\delta\bigl(|a|^{2}+|b|^{2}\bigr)=\delta\bigl(1+\tfrac{\delta}{2}\bigr)|a|^{2}+\delta\bigl(1-\tfrac{\delta}{2}\bigr)|b|^{2}\ \ge\ \tfrac{\delta}{2}\bigl(|a|^{2}+|b|^{2}\bigr). 2 δ 2 ( ∣ a ∣ 2 − ∣ b ∣ 2 ) + δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) = δ ( 1 + 2 δ ) ∣ a ∣ 2 + δ ( 1 − 2 δ ) ∣ b ∣ 2 ≥ 2 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) .
(v) ⟨ Φ ( x ) − Φ ( y ) , w ⟩ = α ⟨ B ( x ) − B ( y ) , x − y ⟩ + α ⟨ L ( x ) − L ( y ) , x − y ⟩ \langle\Phi(x)-\Phi(y),w\rangle=\alpha\langle B(x)-B(y),x-y\rangle+\alpha\langle L(x)-L(y),x-y\rangle ⟨ Φ ( x ) − Φ ( y ) , w ⟩ = α ⟨ B ( x ) − B ( y ) , x − y ⟩ + α ⟨ L ( x ) − L ( y ) , x − y ⟩ . The first summand is nonnegative by Monotone, A A A -Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §monotone and 0 < α 0<\alpha 0 < α . For the second, The Cauchy-Schwarz Inequality in a Real Inner Product Space and the Lipschitz bound give ⟨ L ( x ) − L ( y ) , x − y ⟩ ≥ − ℓ ∣ x − y ∣ 2 \langle L(x)-L(y),x-y\rangle\ge-\ell|x-y|^{2} ⟨ L ( x ) − L ( y ) , x − y ⟩ ≥ − ℓ ∣ x − y ∣ 2 , so, 1 α \tfrac{1}{\alpha} α 1 being positive and ℓ \ell ℓ nonnegative,
⟨ Φ ( x ) − Φ ( y ) , w ⟩ ≥ − ℓ α ∣ x − y ∣ 2 ≥ − ℓ σ . \langle\Phi(x)-\Phi(y),w\rangle\ge-\ell\,\alpha|x-y|^{2}\ge-\ell\,\sigma . ⟨ Φ ( x ) − Φ ( y ) , w ⟩ ≥ − ℓ α ∣ x − y ∣ 2 ≥ − ℓ σ .
(vi) δ ( ⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩ ) = δ ( ⟨ B ( x ) , a ⟩ + ⟨ B ( y ) , b ⟩ ) + δ ( ⟨ L ( x ) , a ⟩ + ⟨ L ( y ) , b ⟩ ) \delta(\langle\Phi(x),a\rangle+\langle\Phi(y),b\rangle)=\delta(\langle B(x),a\rangle+\langle B(y),b\rangle)+\delta(\langle L(x),a\rangle+\langle L(y),b\rangle) δ (⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩) = δ (⟨ B ( x ) , a ⟩ + ⟨ B ( y ) , b ⟩) + δ (⟨ L ( x ) , a ⟩ + ⟨ L ( y ) , b ⟩) . The first summand is nonnegative by Monotone, A A A -Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §a-monotone . For the second, The Cauchy-Schwarz Inequality in a Real Inner Product Space and the second elementary fact give ⟨ L ( x ) , a ⟩ ≥ − ∣ L ( x ) ∣ ∣ a ∣ ≥ − 1 4 ∣ a ∣ 2 − ∣ L ( x ) ∣ 2 \langle L(x),a\rangle\ge-|L(x)|\,|a|\ge-\tfrac{1}{4}|a|^{2}-|L(x)|^{2} ⟨ L ( x ) , a ⟩ ≥ − ∣ L ( x ) ∣ ∣ a ∣ ≥ − 4 1 ∣ a ∣ 2 − ∣ L ( x ) ∣ 2 , while the third elementary fact, the Lipschitz bound and ∣ x ∣ ≤ ∣ x ∣ V |x|\le|x|_{V} ∣ x ∣ ≤ ∣ x ∣ V give
∣ L ( x ) ∣ 2 ≤ ( c L + ℓ ∣ x ∣ ) 2 ≤ 2 c L 2 + 2 ℓ 2 ∣ x ∣ 2 ≤ 2 c L 2 + 2 ℓ 2 ∣ x ∣ V 2 = 2 c L 2 + 4 ℓ 2 h ( x ) , |L(x)|^{2}\le\bigl(c_{L}+\ell|x|\bigr)^{2}\le2c_{L}^{2}+2\ell^{2}|x|^{2}\le2c_{L}^{2}+2\ell^{2}|x|_{V}^{2}=2c_{L}^{2}+4\ell^{2}h(x), ∣ L ( x ) ∣ 2 ≤ ( c L + ℓ ∣ x ∣ ) 2 ≤ 2 c L 2 + 2 ℓ 2 ∣ x ∣ 2 ≤ 2 c L 2 + 2 ℓ 2 ∣ x ∣ V 2 = 2 c L 2 + 4 ℓ 2 h ( x ) ,
and likewise for y y y . Hence
δ ( ⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩ ) ≥ − δ 4 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) − δ ( 4 c L 2 + 4 ℓ 2 ( h ( x ) + h ( y ) ) ) ≥ − δ 4 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) − ( 4 c L 2 + 4 ℓ 2 ) δ ( h ( x ) + h ( y ) + 1 ) , \delta\bigl(\langle\Phi(x),a\rangle+\langle\Phi(y),b\rangle\bigr)\ \ge\ -\tfrac{\delta}{4}\bigl(|a|^{2}+|b|^{2}\bigr)-\delta\Bigl(4c_{L}^{2}+4\ell^{2}\bigl(h(x)+h(y)\bigr)\Bigr)\ \ge\ -\tfrac{\delta}{4}\bigl(|a|^{2}+|b|^{2}\bigr)-\bigl(4c_{L}^{2}+4\ell^{2}\bigr)\,\delta\bigl(h(x)+h(y)+1\bigr), δ ( ⟨ Φ ( x ) , a ⟩ + ⟨ Φ ( y ) , b ⟩ ) ≥ − 4 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) − δ ( 4 c L 2 + 4 ℓ 2 ( h ( x ) + h ( y ) ) ) ≥ − 4 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) − ( 4 c L 2 + 4 ℓ 2 ) δ ( h ( x ) + h ( y ) + 1 ) ,
the last step because 1 ≤ h ( x ) + h ( y ) + 1 1\le h(x)+h(y)+1 1 ≤ h ( x ) + h ( y ) + 1 and h ( x ) + h ( y ) ≤ h ( x ) + h ( y ) + 1 h(x)+h(y)\le h(x)+h(y)+1 h ( x ) + h ( y ) ≤ h ( x ) + h ( y ) + 1 and the coefficients are nonnegative.
(vii) We bound the fourth and the eighth group together. Write t = ∣ x − y ∣ V t=|x-y|_{V} t = ∣ x − y ∣ V , so that their sum is α t 2 − ( g ( x ) − g ( y ) ) \alpha t^{2}-\bigl(g(x)-g(y)\bigr) α t 2 − ( g ( x ) − g ( y ) ) by (ii) . Since x , y ∈ D ( A ) ⊆ V x,y\in D(A)\subseteq V x , y ∈ D ( A ) ⊆ V , the hypotheses on g g g give g ( x ) − g ( y ) ≤ ∣ g ( x ) − g ( y ) ∣ ≤ ω g ( t ) g(x)-g(y)\le|g(x)-g(y)|\le\omega_{g}(t) g ( x ) − g ( y ) ≤ ∣ g ( x ) − g ( y ) ∣ ≤ ω g ( t ) , by claim 3 of Properties of the Absolute Value in an Ordered Field , and ∣ g ( x ) − g ( y ) ∣ ≤ ∣ g ( x ) ∣ + ∣ g ( y ) ∣ ≤ 2 C g |g(x)-g(y)|\le|g(x)|+|g(y)|\le2C_{g} ∣ g ( x ) − g ( y ) ∣ ≤ ∣ g ( x ) ∣ + ∣ g ( y ) ∣ ≤ 2 C g , by claims 2 and 5 of that lemma; so g ( x ) − g ( y ) g(x)-g(y) g ( x ) − g ( y ) is at most both ω g ( t ) \omega_{g}(t) ω g ( t ) and 2 C g 2C_{g} 2 C g and therefore
g ( x ) − g ( y ) ≤ ω ˉ g ( t ) g(x)-g(y)\le\bar{\omega}_{g}(t) g ( x ) − g ( y ) ≤ ω ˉ g ( t )
by The Nondecreasing Envelope of a Truncated Modulus of Continuity §majorant . Note that α t 2 \alpha t^{2} α t 2 is nonnegative, being a product of the positive α \alpha α with a square, and that 0 ≤ ω g ∗ ( σ ) 0\le\omega_{g}^{\ast}(\sigma) 0 ≤ ω g ∗ ( σ ) , ω g ∗ \omega_{g}^{\ast} ω g ∗ being a modulus of continuity.
Suppose first that 2 C g ≤ α t 2 2C_{g}\le\alpha t^{2} 2 C g ≤ α t 2 . Since ω ˉ g ( t ) ≤ 2 C g \bar{\omega}_{g}(t)\le2C_{g} ω ˉ g ( t ) ≤ 2 C g by The Nondecreasing Envelope of a Truncated Modulus of Continuity §modulus , transitivity gives g ( x ) − g ( y ) ≤ α t 2 g(x)-g(y)\le\alpha t^{2} g ( x ) − g ( y ) ≤ α t 2 , so α t 2 − ( g ( x ) − g ( y ) ) \alpha t^{2}-(g(x)-g(y)) α t 2 − ( g ( x ) − g ( y )) is nonnegative and hence at least − ω g ∗ ( σ ) -\omega_{g}^{\ast}(\sigma) − ω g ∗ ( σ ) .
Suppose instead that α t 2 < 2 C g \alpha t^{2}<2C_{g} α t 2 < 2 C g . Multiplying by the positive 1 α \tfrac{1}{\alpha} α 1 gives t 2 < 2 C g 1 α t^{2}<2C_{g}\tfrac{1}{\alpha} t 2 < 2 C g α 1 , while 1 α ≤ σ \tfrac{1}{\alpha}\le\sigma α 1 ≤ σ , the difference being the nonnegative α ∣ x − y ∣ 2 \alpha|x-y|^{2} α ∣ x − y ∣ 2 , and 0 ≤ 2 C g 0\le2C_{g} 0 ≤ 2 C g give 2 C g 1 α ≤ 2 C g σ 2C_{g}\tfrac{1}{\alpha}\le2C_{g}\sigma 2 C g α 1 ≤ 2 C g σ by claim 5 of Elementary Arithmetic in an Ordered Field . Hence t 2 ≤ 2 C g σ t^{2}\le2C_{g}\sigma t 2 ≤ 2 C g σ , and so ω ˉ g ( t ) ≤ ω g ∗ ( σ ) \bar{\omega}_{g}(t)\le\omega_{g}^{\ast}(\sigma) ω ˉ g ( t ) ≤ ω g ∗ ( σ ) by Sums, Nonnegative Multiples, Monotonicity and Quadratic Reparametrisation of Moduli of Continuity §quadratic , the reparametrisation being taken at c = 2 C g c=2C_{g} c = 2 C g . Discarding the nonnegative α t 2 \alpha t^{2} α t 2 ,
α t 2 − ( g ( x ) − g ( y ) ) ≥ − ω ˉ g ( t ) ≥ − ω g ∗ ( σ ) . \alpha t^{2}-\bigl(g(x)-g(y)\bigr)\ \ge\ -\bar{\omega}_{g}(t)\ \ge\ -\omega_{g}^{\ast}(\sigma). α t 2 − ( g ( x ) − g ( y ) ) ≥ − ω ˉ g ( t ) ≥ − ω g ∗ ( σ ) .
In either case
⟨ a − b , w ⟩ − ( g ( x ) − g ( y ) ) ≥ − ω g ∗ ( σ ) . \langle a-b,w\rangle-\bigl(g(x)-g(y)\bigr)\ \ge\ -\omega_{g}^{\ast}(\sigma). ⟨ a − b , w ⟩ − ( g ( x ) − g ( y ) ) ≥ − ω g ∗ ( σ ) .
(viii) The bounds (i), (iii), (iv), (v), (vi) and (vii) account for all eight groups of D D D , the last of them for the fourth and the eighth together. Adding them, the terms δ 2 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) \tfrac{\delta}{2}(|a|^{2}+|b|^{2}) 2 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) of (iv) and − δ 4 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) -\tfrac{\delta}{4}(|a|^{2}+|b|^{2}) − 4 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) of (vi) combine to the nonnegative δ 4 ( ∣ a ∣ 2 + ∣ b ∣ 2 ) \tfrac{\delta}{4}(|a|^{2}+|b|^{2}) 4 δ ( ∣ a ∣ 2 + ∣ b ∣ 2 ) , and we obtain
D ≥ − ω g ∗ ( σ ) − ℓ σ − ( 2 α + 4 c L 2 + 4 ℓ 2 ) δ ( h ( x ) + h ( y ) + 1 ) . D\ \ge\ -\omega_{g}^{\ast}(\sigma)-\ell\,\sigma-\bigl(2\alpha+4c_{L}^{2}+4\ell^{2}\bigr)\,\delta\bigl(h(x)+h(y)+1\bigr). D ≥ − ω g ∗ ( σ ) − ℓ σ − ( 2 α + 4 c L 2 + 4 ℓ 2 ) δ ( h ( x ) + h ( y ) + 1 ) .
Since 1 < α 1<\alpha 1 < α and 4 c L 2 + 4 ℓ 2 4c_{L}^{2}+4\ell^{2} 4 c L 2 + 4 ℓ 2 is nonnegative, 2 α + 4 c L 2 + 4 ℓ 2 ≤ 2 α + ( 4 c L 2 + 4 ℓ 2 ) α = K α 2\alpha+4c_{L}^{2}+4\ell^{2}\le2\alpha+(4c_{L}^{2}+4\ell^{2})\alpha=K\alpha 2 α + 4 c L 2 + 4 ℓ 2 ≤ 2 α + ( 4 c L 2 + 4 ℓ 2 ) α = K α , so the right-hand side is at least − ω 1 ( σ ) − ω 2 ( δ ( h ( x ) + h ( y ) + 1 ) , α ) -\omega_{1}(\sigma)-\omega_{2}(\delta(h(x)+h(y)+1),\alpha) − ω 1 ( σ ) − ω 2 ( δ ( h ( x ) + h ( y ) + 1 ) , α ) . This is the inequality required by The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple §pair , so ( ω 1 , ω 2 ) (\omega_{1},\omega_{2}) ( ω 1 , ω 2 ) is a structure pair for F F F at R R R ; as R R R was an arbitrary positive real, F F F satisfies the first-order structure condition by The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple §structure .
Claim 4, a bound on the form operator over the admissible sets. Let δ , R ∈ R \delta,R\in\mathbb{R} δ , R ∈ R satisfy 0 < δ < 1 0<\delta<1 0 < δ < 1 and 0 < R 0<R 0 < R . Let ρ \rho ρ be the nonnegative real with ρ 2 = 2 R \rho^{2}=2R ρ 2 = 2 R , given by Existence and Uniqueness of the Nonnegative Square Root . If ( z , r , p , X ) ∈ W (z,r,p,X)\in\mathcal{W} ( z , r , p , X ) ∈ W is R R R -bounded then h ( z ) < R h(z)<R h ( z ) < R , so ∣ z ∣ V 2 = 2 h ( z ) < ρ 2 |z|_{V}^{2}=2h(z)<\rho^{2} ∣ z ∣ V 2 = 2 h ( z ) < ρ 2 and therefore ∣ z ∣ V ≤ ρ |z|_{V}\le\rho ∣ z ∣ V ≤ ρ by claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field and trichotomy, and ∣ z ∣ ≤ ρ |z|\le\rho ∣ z ∣ ≤ ρ . Let β \beta β be a bound for B B B on the set of v ∈ V v\in V v ∈ V with ∣ v ∣ V ≤ ρ |v|_{V}\le\rho ∣ v ∣ V ≤ ρ , as provided by Monotone, A A A -Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §bounded , put μ = c L + ℓ ρ \mu=c_{L}+\ell\rho μ = c L + ℓ ρ and N = β + μ N=\beta+\mu N = β + μ ; then ∣ Φ ( z ) ∣ ≤ N |\Phi(z)|\le N ∣Φ ( z ) ∣ ≤ N for every such z z z , by The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle and the bound on ∣ L ∣ |L| ∣ L ∣ .
Let ξ = ( x , r , p , X ) \xi=(x,r,p,X) ξ = ( x , r , p , X ) be R R R -bounded. From ( ∗ ) (*) ( ∗ ) , using 1 2 ∣ p ∣ 2 ≥ 0 \tfrac{1}{2}|p|^{2}\ge0 2 1 ∣ p ∣ 2 ≥ 0 , The Cauchy-Schwarz Inequality in a Real Inner Product Space , ∣ p ∣ < R |p|<R ∣ p ∣ < R , 1 + δ ≤ 2 1+\delta\le2 1 + δ ≤ 2 , the second elementary fact in the form ⟨ L ( x ) , a ⟩ ≥ − 1 4 ∣ a ∣ 2 − ∣ L ( x ) ∣ 2 \langle L(x),a\rangle\ge-\tfrac{1}{4}|a|^{2}-|L(x)|^{2} ⟨ L ( x ) , a ⟩ ≥ − 4 1 ∣ a ∣ 2 − ∣ L ( x ) ∣ 2 , Monotone, A A A -Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §a-monotone , 0 ≤ h ( x ) 0\le h(x) 0 ≤ h ( x ) , − R ≤ r -R\le r − R ≤ r and ∣ g ( x ) ∣ ≤ C g |g(x)|\le C_{g} ∣ g ( x ) ∣ ≤ C g ,
F δ − ( ξ ) ≥ ( 1 + δ ) 2 − 1 2 ∣ a ∣ 2 − 2 R ∣ a ∣ − N R − δ 4 ∣ a ∣ 2 − μ 2 − λ 0 R − C g ≥ 3 δ 4 ∣ a ∣ 2 − 2 R ∣ a ∣ − C − , F^{-}_{\delta}(\xi)\ \ge\ \tfrac{(1+\delta)^{2}-1}{2}|a|^{2}-2R|a|-NR-\tfrac{\delta}{4}|a|^{2}-\mu^{2}-\lambda_{0}R-C_{g}\ \ge\ \tfrac{3\delta}{4}|a|^{2}-2R|a|-C_{-}, F δ − ( ξ ) ≥ 2 ( 1 + δ ) 2 − 1 ∣ a ∣ 2 − 2 R ∣ a ∣ − NR − 4 δ ∣ a ∣ 2 − μ 2 − λ 0 R − C g ≥ 4 3 δ ∣ a ∣ 2 − 2 R ∣ a ∣ − C − ,
where C − = N R + μ 2 + λ 0 R + C g C_{-}=NR+\mu^{2}+\lambda_{0}R+C_{g} C − = NR + μ 2 + λ 0 R + C g ; here ( 1 + δ ) 2 − 1 2 = δ + δ 2 2 ≥ δ \tfrac{(1+\delta)^{2}-1}{2}=\delta+\tfrac{\delta^{2}}{2}\ge\delta 2 ( 1 + δ ) 2 − 1 = δ + 2 δ 2 ≥ δ . Similarly, let η = ( y , s , p ′ , X ′ ) \eta=(y,s,p',X') η = ( y , s , p ′ , X ′ ) be R R R -bounded. From ( ∗ ∗ ) (**) ( ∗ ∗ ) , using 1 2 ∣ p ′ ∣ 2 ≤ 1 2 R 2 \tfrac{1}{2}|p'|^{2}\le\tfrac{1}{2}R^{2} 2 1 ∣ p ′ ∣ 2 ≤ 2 1 R 2 , The Cauchy-Schwarz Inequality in a Real Inner Product Space , 1 − δ ≤ 1 1-\delta\le1 1 − δ ≤ 1 , ∣ Φ ( y ) ∣ ≤ N |\Phi(y)|\le N ∣Φ ( y ) ∣ ≤ N , 0 ≤ h ( y ) 0\le h(y) 0 ≤ h ( y ) , s ≤ R s\le R s ≤ R and − g ( y ) ≤ C g -g(y)\le C_{g} − g ( y ) ≤ C g ,
F δ + ( η ) ≤ − 1 − ( 1 − δ ) 2 2 ∣ b ∣ 2 + ( R + N ) ∣ b ∣ + C + ≤ − δ 2 ∣ b ∣ 2 + ( R + N ) ∣ b ∣ + C + , F^{+}_{\delta}(\eta)\ \le\ -\tfrac{1-(1-\delta)^{2}}{2}|b|^{2}+(R+N)|b|+C_{+}\ \le\ -\tfrac{\delta}{2}|b|^{2}+(R+N)|b|+C_{+}, F δ + ( η ) ≤ − 2 1 − ( 1 − δ ) 2 ∣ b ∣ 2 + ( R + N ) ∣ b ∣ + C + ≤ − 2 δ ∣ b ∣ 2 + ( R + N ) ∣ b ∣ + C + ,
where C + = 1 2 R 2 + N R + λ 0 R + C g C_{+}=\tfrac{1}{2}R^{2}+NR+\lambda_{0}R+C_{g} C + = 2 1 R 2 + NR + λ 0 R + C g ; here 1 − ( 1 − δ ) 2 2 = δ − δ 2 2 ≥ δ 2 \tfrac{1-(1-\delta)^{2}}{2}=\delta-\tfrac{\delta^{2}}{2}\ge\tfrac{\delta}{2} 2 1 − ( 1 − δ ) 2 = δ − 2 δ 2 ≥ 2 δ because δ < 1 \delta<1 δ < 1 .
By the second elementary fact, 2 R ∣ a ∣ ≤ 3 δ 8 ∣ a ∣ 2 + 8 R 2 3 δ 2R|a|\le\tfrac{3\delta}{8}|a|^{2}+\tfrac{8R^{2}}{3\delta} 2 R ∣ a ∣ ≤ 8 3 δ ∣ a ∣ 2 + 3 δ 8 R 2 and ( R + N ) ∣ b ∣ ≤ δ 4 ∣ b ∣ 2 + ( R + N ) 2 δ (R+N)|b|\le\tfrac{\delta}{4}|b|^{2}+\tfrac{(R+N)^{2}}{\delta} ( R + N ) ∣ b ∣ ≤ 4 δ ∣ b ∣ 2 + δ ( R + N ) 2 . Hence the two displays give
F δ − ( ξ ) ≥ 3 δ 8 ∣ a ∣ 2 − E , F δ + ( η ) ≤ − δ 4 ∣ b ∣ 2 + E , F^{-}_{\delta}(\xi)\ \ge\ \tfrac{3\delta}{8}|a|^{2}-E,\qquad F^{+}_{\delta}(\eta)\ \le\ -\tfrac{\delta}{4}|b|^{2}+E, F δ − ( ξ ) ≥ 8 3 δ ∣ a ∣ 2 − E , F δ + ( η ) ≤ − 4 δ ∣ b ∣ 2 + E ,
where E = 8 R 2 3 δ + ( R + N ) 2 δ + C − + C + E=\tfrac{8R^{2}}{3\delta}+\tfrac{(R+N)^{2}}{\delta}+C_{-}+C_{+} E = 3 δ 8 R 2 + δ ( R + N ) 2 + C − + C + ; in particular F δ − ( ξ ) ≥ − E F^{-}_{\delta}(\xi)\ge-E F δ − ( ξ ) ≥ − E and F δ + ( η ) ≤ E F^{+}_{\delta}(\eta)\le E F δ + ( η ) ≤ E for all R R R -bounded ξ \xi ξ and η \eta η .
Now let ξ = ( x , r , p , X ) ∈ S δ , R − \xi=(x,r,p,X)\in S^{-}_{\delta,R} ξ = ( x , r , p , X ) ∈ S δ , R − . By Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets §admissible there is an R R R -bounded η \eta η with F δ − ( ξ ) − F δ + ( η ) < R F^{-}_{\delta}(\xi)-F^{+}_{\delta}(\eta)<R F δ − ( ξ ) − F δ + ( η ) < R , so 3 δ 8 ∣ a ∣ 2 − E ≤ F δ − ( ξ ) < R + F δ + ( η ) ≤ R + E \tfrac{3\delta}{8}|a|^{2}-E\le F^{-}_{\delta}(\xi)<R+F^{+}_{\delta}(\eta)\le R+E 8 3 δ ∣ a ∣ 2 − E ≤ F δ − ( ξ ) < R + F δ + ( η ) ≤ R + E and therefore ∣ a ∣ 2 < 8 ( R + 2 E ) 3 δ |a|^{2}<\tfrac{8(R+2E)}{3\delta} ∣ a ∣ 2 < 3 δ 8 ( R + 2 E ) . Similarly, if η = ( y , s , p ′ , X ′ ) ∈ S δ , R + \eta=(y,s,p',X')\in S^{+}_{\delta,R} η = ( y , s , p ′ , X ′ ) ∈ S δ , R + there is an R R R -bounded ξ \xi ξ with F δ − ( ξ ) − F δ + ( η ) < R F^{-}_{\delta}(\xi)-F^{+}_{\delta}(\eta)<R F δ − ( ξ ) − F δ + ( η ) < R , so − δ 4 ∣ b ∣ 2 + E ≥ F δ + ( η ) > F δ − ( ξ ) − R ≥ − E − R -\tfrac{\delta}{4}|b|^{2}+E\ge F^{+}_{\delta}(\eta)>F^{-}_{\delta}(\xi)-R\ge-E-R − 4 δ ∣ b ∣ 2 + E ≥ F δ + ( η ) > F δ − ( ξ ) − R ≥ − E − R and therefore ∣ b ∣ 2 < 4 ( R + 2 E ) δ |b|^{2}<\tfrac{4(R+2E)}{\delta} ∣ b ∣ 2 < δ 4 ( R + 2 E ) . Let Λ \Lambda Λ be the nonnegative real whose square is the larger of 8 ( R + 2 E ) 3 δ \tfrac{8(R+2E)}{3\delta} 3 δ 8 ( R + 2 E ) and 4 ( R + 2 E ) δ \tfrac{4(R+2E)}{\delta} δ 4 ( R + 2 E ) , again by Existence and Uniqueness of the Nonnegative Square Root . Then ∣ A x ∣ ≤ Λ |Ax|\le\Lambda ∣ A x ∣ ≤ Λ whenever ( x , r , p , X ) (x,r,p,X) ( x , r , p , X ) lies in S δ , R − S^{-}_{\delta,R} S δ , R − or in S δ , R + S^{+}_{\delta,R} S δ , R + , by claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field and trichotomy.
Claim 4, the shift modulus. Put c = R + 2 Λ + N c=R+2\Lambda+N c = R + 2Λ + N and let ω \omega ω be the function on the nonnegative reals with ω ( t ) = c t + 1 2 t 2 \omega(t)=c\,t+\tfrac{1}{2}t^{2} ω ( t ) = c t + 2 1 t 2 . It is nonnegative there. Given a positive ε \varepsilon ε , let δ 0 \delta_{0} δ 0 be the lesser of 1 1 1 and ε c + 1 \tfrac{\varepsilon}{c+1} c + 1 ε , which is positive; every nonnegative t ≤ δ 0 t\le\delta_{0} t ≤ δ 0 satisfies t ≤ 1 t\le1 t ≤ 1 , hence t 2 ≤ t t^{2}\le t t 2 ≤ t and ω ( t ) ≤ ( c + 1 ) t ≤ ε \omega(t)\le(c+1)t\le\varepsilon ω ( t ) ≤ ( c + 1 ) t ≤ ε . So ω \omega ω is a modulus of continuity. It is also nondecreasing on the nonnegative reals: for 0 ≤ s ≤ t 0\le s\le t 0 ≤ s ≤ t we have c s ≤ c t c\,s\le c\,t c s ≤ c t by Linear Moduli of Continuity §monotone , and s 2 ≤ t 2 s^{2}\le t^{2} s 2 ≤ t 2 by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field , whence 1 2 s 2 ≤ 1 2 t 2 \tfrac{1}{2}s^{2}\le\tfrac{1}{2}t^{2} 2 1 s 2 ≤ 2 1 t 2 by claim 5 of Elementary Arithmetic in an Ordered Field ; adding the two inequalities by claims 3 and 2 of that lemma gives ω ( s ) ≤ ω ( t ) \omega(s)\le\omega(t) ω ( s ) ≤ ω ( t ) .
Let q ∈ H q\in H q ∈ H and Y ∈ S y m ( H ) Y\in\mathrm{Sym}(H) Y ∈ Sym ( H ) . Let ( x , r , p , X ) ∈ S δ , R − (x,r,p,X)\in S^{-}_{\delta,R} ( x , r , p , X ) ∈ S δ , R − and put P = p + δ a P=p+\delta a P = p + δ a , so that ∣ P ∣ ≤ R + δ Λ ≤ R + Λ |P|\le R+\delta\Lambda\le R+\Lambda ∣ P ∣ ≤ R + δ Λ ≤ R + Λ by The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle . Since F F F , and hence each of its shifts, does not depend on its fourth argument, Elementary Identities in a Real Inner Product Space §expansion and The Cauchy-Schwarz Inequality in a Real Inner Product Space give
F δ − ( x , r , p + q , X + Y ) − F δ − ( x , r , p , X ) = ⟨ P , q ⟩ + 1 2 ∣ q ∣ 2 + ⟨ a + Φ ( x ) , q ⟩ ≤ ( ∣ P ∣ + ∣ a ∣ + ∣ Φ ( x ) ∣ ) ∣ q ∣ + 1 2 ∣ q ∣ 2 ≤ ω ( ∣ q ∣ ) , F^{-}_{\delta}(x,r,p+q,X+Y)-F^{-}_{\delta}(x,r,p,X)=\langle P,q\rangle+\tfrac{1}{2}|q|^{2}+\langle a+\Phi(x),q\rangle\le\bigl(|P|+|a|+|\Phi(x)|\bigr)|q|+\tfrac{1}{2}|q|^{2}\le\omega(|q|), F δ − ( x , r , p + q , X + Y ) − F δ − ( x , r , p , X ) = ⟨ P , q ⟩ + 2 1 ∣ q ∣ 2 + ⟨ a + Φ ( x ) , q ⟩ ≤ ( ∣ P ∣ + ∣ a ∣ + ∣Φ ( x ) ∣ ) ∣ q ∣ + 2 1 ∣ q ∣ 2 ≤ ω ( ∣ q ∣ ) ,
because ∣ P ∣ + ∣ a ∣ + ∣ Φ ( x ) ∣ ≤ ( R + Λ ) + Λ + N = c |P|+|a|+|\Phi(x)|\le(R+\Lambda)+\Lambda+N=c ∣ P ∣ + ∣ a ∣ + ∣Φ ( x ) ∣ ≤ ( R + Λ ) + Λ + N = c . As ω \omega ω is nondecreasing and 0 ≤ ∥ Y ∥ 0\le\lVert Y\rVert 0 ≤ ∥ Y ∥ , we get ω ( ∣ q ∣ ) ≤ ω ( ∣ q ∣ + ∥ Y ∥ ) \omega(|q|)\le\omega(|q|+\lVert Y\rVert) ω ( ∣ q ∣ ) ≤ ω ( ∣ q ∣ + ∥ Y ∥) , which is the first requirement of The Shift-Continuity Condition on Admissible Test Data §modulus . Likewise, for ( y , s , p ′ , X ′ ) ∈ S δ , R + (y,s,p',X')\in S^{+}_{\delta,R} ( y , s , p ′ , X ′ ) ∈ S δ , R + , putting P ′ = p ′ − δ b P'=p'-\delta b P ′ = p ′ − δ b ,
F δ + ( y , s , p ′ + q , X ′ + Y ) − F δ + ( y , s , p ′ , X ′ ) = ⟨ P ′ , q ⟩ + 1 2 ∣ q ∣ 2 + ⟨ b + Φ ( y ) , q ⟩ ≥ − ( ∣ P ′ ∣ + ∣ b ∣ + ∣ Φ ( y ) ∣ ) ∣ q ∣ ≥ − ω ( ∣ q ∣ + ∥ Y ∥ ) , F^{+}_{\delta}(y,s,p'+q,X'+Y)-F^{+}_{\delta}(y,s,p',X')=\langle P',q\rangle+\tfrac{1}{2}|q|^{2}+\langle b+\Phi(y),q\rangle\ge-\bigl(|P'|+|b|+|\Phi(y)|\bigr)|q|\ge-\omega(|q|+\lVert Y\rVert), F δ + ( y , s , p ′ + q , X ′ + Y ) − F δ + ( y , s , p ′ , X ′ ) = ⟨ P ′ , q ⟩ + 2 1 ∣ q ∣ 2 + ⟨ b + Φ ( y ) , q ⟩ ≥ − ( ∣ P ′ ∣ + ∣ b ∣ + ∣Φ ( y ) ∣ ) ∣ q ∣ ≥ − ω ( ∣ q ∣ + ∥ Y ∥) ,
where 1 2 ∣ q ∣ 2 \tfrac{1}{2}|q|^{2} 2 1 ∣ q ∣ 2 was discarded as nonnegative. This is the second requirement. Hence ω \omega ω is a shift modulus for F F F at ( δ , R ) (\delta,R) ( δ , R ) , and as δ \delta δ and R R R were arbitrary, F F F satisfies the shift-continuity condition by The Shift-Continuity Condition on Admissible Test Data §continuity .
Claim 5. By claims 1, 2, 3 and 4 the operator F F F is a first-order second-order equation operator on H H H that is locally strictly proper and satisfies the first-order structure condition and the shift-continuity condition, which are the hypotheses of A Comparison Principle on a Hilbert Triple under the First-Order Structure Condition §comparison ; applying that theorem to u u u , v v v and C C C gives u ( x ) ≤ v ( x ) u(x)\le v(x) u ( x ) ≤ v ( x ) for every x ∈ V x\in V x ∈ V .