TheoremBase

0 <= Gamma <= IHI_H gives 0 <= Gamma(p,p) <= |p|^2 and |Gamma(p,q)| <= |p||q|. Ellipticity, properness and tail-insensitivity see only the trace and zeroth-order terms. In the structure condition the cross term delta Gamma(w, Ax+Ay) costs (delta/32)(|Ax|^2+|Ay|^2) + 64 alpha2alpha^2 delta (h(x)+h(y)); with the diagonal and Lipschitz losses it is dominated by the dissipation delta(|Ax|^2+|Ay|^2), giving K = 64+4c_L^2+4l^2. Coercivity on the admissible sets bounds |Ax|, yielding a shift modulus; comparison follows from the comparison theorem.

Proof

Each result cited is universally quantified over the data in its own statement. Throughout, x,y∈D(A)x,y\in D(A), and we write a=Axa=Ax, b=Ayb=Ay and Φ(z)=B(z)+L(z)\Phi(z)=B(z)+L(z) for z∈Vz\in V; norms and pairings without a subscript are those of HH. By The Penalty Function h=12∣⋅∣V2h=\tfrac12|\cdot|_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) for z∈Vz\in V, and 2h(z)=∣z∣V22h(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} for z∈Vz\in V. By Elementary Properties of a Hilbert Triple: the Embedding, the Riesz Map and the Form Operator §symmetric, ⟨Az,ζ⟩H=⟨z,ζ⟩V\langle Az,\zeta\rangle_{H}=\langle z,\zeta\rangle_{V} for z∈D(A)z\in D(A) and ζ∈V\zeta\in V. For Y∈Sym(H)Y\in\mathrm{Sym}(H) we write Y∣VY|_{V} for its restriction to VV. The standing hypothesis 0≤ν0\le\nu is used throughout, as is 0≤σ(f)0\le\sigma(f), which holds by Square-Summable Sequences in the Form Space of a Hilbert Triple and the Trace of a Form along Them §square-summable; the trace Trf\mathrm{Tr}_{f} is used only through Elementary Properties of the Trace of a Form along a Square-Summable Sequence.

Since LL is Lipschitz with constant ℓ\ell, ∣L(z)−L(ζ)∣≤ℓ∣z−ζ∣|L(z)-L(\zeta)|\le\ell|z-\zeta| for z,ζ∈Hz,\zeta\in H, and taking ζ=0H\zeta=0_{H} and using The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle gives

∣L(z)∣≤cL+ℓ∣z∣for every z∈H.|L(z)|\le c_{L}+\ell|z|\qquad\text{for every }z\in H .

We use the following three elementary facts. First, Elementary Identities in a Real Inner Product Space §expansion gives ∣c+u∣2=∣c∣2+2⟨c,u⟩+∣u∣2|c+u|^{2}=|c|^{2}+2\langle c,u\rangle+|u|^{2} for c,u∈Hc,u\in H. Secondly, for real c>0c>0 and s,ts,t with 0≤s0\le s and 0≤t0\le t, expanding 0≤1c(c s−t)20\le\tfrac{1}{c}(c\,s-t)^{2} gives 2st≤c s2+t2c2st\le c\,s^{2}+\tfrac{t^{2}}{c}; we use it as st≤14s2+t2st\le\tfrac{1}{4}s^{2}+t^{2} (the case c=12c=\tfrac{1}{2}) and in the displayed forms below. Thirdly, (s+t)2≤2s2+2t2(s+t)^{2}\le2s^{2}+2t^{2} for real s,ts,t, by Products and Sums of Weighted Square-Summable Sequences of Real Numbers §pointwise.

We also use three facts about Γ\Gamma: for all p,q∈Hp,q\in H and c∈Rc\in\mathbb{R},

0≤Γ(p,p)≤∣p∣2,∣Γ(p,q)∣≤∣p∣ ∣q∣,Γ(p+cq,p+cq)=Γ(p,p)+2c Γ(p,q)+c2 Γ(q,q).0\le\Gamma(p,p)\le|p|^{2},\qquad |\Gamma(p,q)|\le|p|\,|q|,\qquad \Gamma(p+cq,p+cq)=\Gamma(p,p)+2c\,\Gamma(p,q)+c^{2}\,\Gamma(q,q).

The first is the hypothesis 0Sym⪯Γ⪯IH0_{\mathrm{Sym}}\preceq\Gamma\preceq I_{H} read through Bounded Symmetric Bilinear Forms on a Real Inner Product Space: Norm, Order, Identity Form and Restriction §order, since 0Sym(p,p)=00_{\mathrm{Sym}}(p,p)=0 and IH(p,p)=⟨p,p⟩=∣p∣2I_{H}(p,p)=\langle p,p\rangle=|p|^{2} by Hilbert Triples: Standing Notation and Background §restriction and Bounded Symmetric Bilinear Forms on a Real Inner Product Space: Norm, Order, Identity Form and Restriction §identity. For the second, −IH⪯0Sym-I_{H}\preceq0_{\mathrm{Sym}} because −∣p∣2≤0-|p|^{2}\le0 for every p∈Hp\in H, so −IH⪯Γ⪯IH-I_{H}\preceq\Gamma\preceq I_{H} by the transitivity in Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity §order-partial; hence ∥Γ∥≤1\lVert\Gamma\rVert\le1 by Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity §order-norm, and ∣Γ(p,q)∣≤∥Γ∥ ∣p∣ ∣q∣≤∣p∣ ∣q∣|\Gamma(p,q)|\le\lVert\Gamma\rVert\,|p|\,|q|\le|p|\,|q| by Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity §bound. The third follows from the symmetry, additivity and homogeneity of Γ\Gamma in Bounded Symmetric Bilinear Forms on a Real Inner Product Space: Norm, Order, Identity Form and Restriction §form.

Claim 1. The values of FF are real numbers and its domain is D(A)×R×H×Sym(V)D(A)\times\mathbb{R}\times H\times\mathrm{Sym}(V), which with W=D(A)W=D(A) is what Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts §operator requires of a second-order equation operator on HH. For degenerate ellipticity, let x∈D(A)x\in D(A), r∈Rr\in\mathbb{R}, p∈Hp\in H and X,Y∈Sym(V)X,Y\in\mathrm{Sym}(V) with X⪯YX\preceq Y. Every term of the defining expression other than −ν2TrfX-\tfrac{\nu}{2}\mathrm{Tr}_{f}X is independent of the fourth argument, and TrfX≤TrfY\mathrm{Tr}_{f}X\le\mathrm{Tr}_{f}Y by Elementary Properties of the Trace of a Form along a Square-Summable Sequence §monotone, so

F(x,r,p,Y)−F(x,r,p,X)=−ν2(TrfY−TrfX)≤0,F(x,r,p,Y)-F(x,r,p,X)=-\tfrac{\nu}{2}\bigl(\mathrm{Tr}_{f}Y-\mathrm{Tr}_{f}X\bigr)\le0,

because ν2\tfrac{\nu}{2} and TrfY−TrfX\mathrm{Tr}_{f}Y-\mathrm{Tr}_{f}X are nonnegative, by claim 5 of Elementary Arithmetic in an Ordered Field and claim 4 of Elementary Order Arithmetic in an Ordered Field. Thus F(x,r,p,Y)≤F(x,r,p,X)F(x,r,p,Y)\le F(x,r,p,X), which is Degenerate Elliptic Second-Order Equation Operator on a Hilbert Triple §elliptic.

Claim 2. Let RR be positive, x∈D(A)x\in D(A), p∈Hp\in H, X∈Sym(V)X\in\mathrm{Sym}(V) and r,s∈Rr,s\in\mathbb{R} with −R≤s≤r≤R-R\le s\le r\le R. Every term of FF other than λ0r\lambda_{0}r is independent of the second argument, so

F(x,r,p,X)−F(x,s,p,X)=λ0r−λ0s=λ0(r−s),F(x,r,p,X)-F(x,s,p,X)=\lambda_{0}r-\lambda_{0}s=\lambda_{0}(r-s),

and in particular λ0(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). As λ0\lambda_{0} is positive, this is the requirement of Locally Strictly Proper Second-Order Equation Operator on a Hilbert Triple §constant; since RR was an arbitrary positive real, FF 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} satisfy 0<δ<10<\delta<1. By Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts §shifted, the δ\delta-shifts are given by

Fδ−(x,r,p,X)=λ0(r+δh(x))−ν2 Trf(X∣V+δIV)+12 Γ(p+δa,p+δa)+⟨a+Φ(x),p+δa⟩−g(x),F^{-}_{\delta}(x,r,p,X)=\lambda_{0}\bigl(r+\delta h(x)\bigr)-\tfrac{\nu}{2}\,\mathrm{Tr}_{f}\bigl(X|_{V}+\delta I_{V}\bigr)+\tfrac12\,\Gamma(p+\delta a,p+\delta a)+\langle a+\Phi(x),p+\delta a\rangle-g(x), Fδ+(y,s,p′,X′)=λ0(s−δh(y))−ν2 Trf(X′∣V−δIV)+12 Γ(p′−δb,p′−δb)+⟨b+Φ(y),p′−δb⟩−g(y),F^{+}_{\delta}(y,s,p',X')=\lambda_{0}\bigl(s-\delta h(y)\bigr)-\tfrac{\nu}{2}\,\mathrm{Tr}_{f}\bigl(X'|_{V}-\delta I_{V}\bigr)+\tfrac12\,\Gamma(p'-\delta b,p'-\delta b)+\langle b+\Phi(y),p'-\delta b\rangle-g(y),

for x,y∈D(A)x,y\in D(A), r,s∈Rr,s\in\mathbb{R}, p,p′∈Hp,p'\in H and X,X′∈Sym(H)X,X'\in\mathrm{Sym}(H). By Elementary Properties of the Trace of a Form along a Square-Summable Sequence §linear and Elementary Properties of the Trace of a Form along a Square-Summable Sequence §identity,

Trf(X∣V+δIV)=Trf(X∣V)+δ σ(f),Trf(X′∣V−δIV)=Trf(X′∣V)−δ σ(f).\mathrm{Tr}_{f}\bigl(X|_{V}+\delta I_{V}\bigr)=\mathrm{Tr}_{f}(X|_{V})+\delta\,\sigma(f), \qquad \mathrm{Tr}_{f}\bigl(X'|_{V}-\delta I_{V}\bigr)=\mathrm{Tr}_{f}(X'|_{V})-\delta\,\sigma(f).

Claim 3, the two moduli. By The Nondecreasing Envelope of a Truncated Modulus of Continuity §modulus the function ωˉg\bar{\omega}_{g} is a modulus of continuity satisfying 0≤ωˉg(t)≤2Cg0\le\bar{\omega}_{g}(t)\le2C_{g} for every nonnegative tt; as 2Cg2C_{g} is nonnegative, its quadratic reparametrisation ωg∗\omega_{g}^{\ast} at 2Cg2C_{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↦ℓtt\mapsto\ell t is a modulus of continuity, since 0≤ℓ0\le\ell; so ω1\omega_{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 the number Kα2+ν σ(f)K\alpha^{2}+\nu\,\sigma(f) is nonnegative, being the sum of a product of positive numbers and a product of two nonnegative numbers, so t↦(Kα2+ν σ(f)) tt\mapsto(K\alpha^{2}+\nu\,\sigma(f))\,t is a modulus of continuity by Linear Moduli of Continuity §modulus.

Claim 3, the inequality. Let RR be positive, let x,y∈D(A)x,y\in D(A), let r∈Rr\in\mathbb{R} with −R≤r≤R-R\le r\le R, let α,δ∈R\alpha,\delta\in\mathbb{R} with 1<α1<\alpha and 0<δ<10<\delta<1, and let (X,Y)(X,Y) be a pair of members of Sym(H)\mathrm{Sym}(H) admitted at α\alpha. Put w=α(x−y)w=\alpha(x-y) and τ=α∣x−y∣2+1α\tau=\alpha|x-y|^{2}+\tfrac{1}{\alpha}, and let D=Fδ−(x,r,w,X)−Fδ+(y,r,w,Y)D=F^{-}_{\delta}(x,r,w,X)-F^{+}_{\delta}(y,r,w,Y). Expanding the two shift formulas of the previous paragraph, using the third fact about Γ\Gamma on the two quadratic terms in the gradient, whose terms 12Γ(w,w)\tfrac12\Gamma(w,w) cancel, and using the two trace identities recorded there,

D=λ0δ(h(x)+h(y))+ν2(Trf(Y∣V)−Trf(X∣V))−νδ σ(f)+δ Γ(w,a+b)+δ22(Γ(a,a)−Γ(b,b))+⟨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)+\tfrac{\nu}{2}\bigl(\mathrm{Tr}_{f}(Y|_{V})-\mathrm{Tr}_{f}(X|_{V})\bigr)-\nu\delta\,\sigma(f)+\delta\,\Gamma(w,a+b)+\tfrac{\delta^{2}}{2}\bigl(\Gamma(a,a)-\Gamma(b,b)\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).

We bound the ten groups in turn, taking the sixth and the tenth together in (vii).

(i) 0≤λ0δ(h(x)+h(y))0\le\lambda_{0}\delta(h(x)+h(y)), all three factors being nonnegative.

(i-a) Being admitted at α\alpha, the pair satisfies X⪯YX\preceq Y; hence X∣V⪯Y∣VX|_{V}\preceq Y|_{V} by claim 10 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity and therefore Trf(X∣V)≤Trf(Y∣V)\mathrm{Tr}_{f}(X|_{V})\le\mathrm{Tr}_{f}(Y|_{V}) by Elementary Properties of the Trace of a Form along a Square-Summable Sequence §monotone. As ν2\tfrac{\nu}{2} is nonnegative,

0≤ν2(Trf(Y∣V)−Trf(X∣V)).0\le\tfrac{\nu}{2}\bigl(\mathrm{Tr}_{f}(Y|_{V})-\mathrm{Tr}_{f}(X|_{V})\bigr).

(i-b) Since 0≤h(x)+h(y)0\le h(x)+h(y) we have δ≤δ(h(x)+h(y)+1)\delta\le\delta(h(x)+h(y)+1), and ν σ(f)\nu\,\sigma(f) is nonnegative, so by claim 5 of Elementary Arithmetic in an Ordered Field and claim 4 of Elementary Order Arithmetic in an Ordered Field,

−νδ σ(f) ≥ −ν σ(f)⋅δ(h(x)+h(y)+1).-\nu\delta\,\sigma(f)\ \ge\ -\nu\,\sigma(f)\cdot\delta\bigl(h(x)+h(y)+1\bigr).

(ii) Since x−y∈Vx-y\in V, the symmetry identity gives ⟨a−b,w⟩=α(⟨x,x−y⟩V−⟨y,x−y⟩V)=α∣x−y∣V2\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}, which is nonnegative. This term is not discarded: it is combined with the tenth group in (vii), where it absorbs the oscillation of gg.

(iii) By the second fact about Γ\Gamma and The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle, δ Γ(w,a+b)≥−δ∣w∣ ∣a+b∣≥−δ∣w∣ ∣a∣−δ∣w∣ ∣b∣\delta\,\Gamma(w,a+b)\ge-\delta|w|\,|a+b|\ge-\delta|w|\,|a|-\delta|w|\,|b|, and the second elementary fact with c=116c=\tfrac{1}{16} gives ∣w∣ ∣a∣≤132∣a∣2+8∣w∣2|w|\,|a|\le\tfrac{1}{32}|a|^{2}+8|w|^{2} and ∣w∣ ∣b∣≤132∣b∣2+8∣w∣2|w|\,|b|\le\tfrac{1}{32}|b|^{2}+8|w|^{2}. By Elementary Identities in a Real Inner Product Space §homogeneity and 0<α0<\alpha, by Elementary Identities in a Real Inner Product Space §parallelogram together with 0≤∣x+y∣20\le|x+y|^{2}, and by ∣x∣≤∣x∣V|x|\le|x|_{V}, ∣y∣≤∣y∣V|y|\le|y|_{V} with claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field,

∣w∣2=α2∣x−y∣2≤α2(2∣x∣2+2∣y∣2)≤2α2(∣x∣V2+∣y∣V2)=4α2(h(x)+h(y)).|w|^{2}=\alpha^{2}|x-y|^{2}\le\alpha^{2}\bigl(2|x|^{2}+2|y|^{2}\bigr)\le2\alpha^{2}\bigl(|x|_{V}^{2}+|y|_{V}^{2}\bigr)=4\alpha^{2}\bigl(h(x)+h(y)\bigr).

Hence, as h(x)+h(y)≤h(x)+h(y)+1h(x)+h(y)\le h(x)+h(y)+1 and the coefficients are nonnegative,

δ Γ(w,a+b) ≥ −δ32(∣a∣2+∣b∣2)−16δ∣w∣2 ≥ −δ32(∣a∣2+∣b∣2)−64α2⋅δ(h(x)+h(y)+1).\delta\,\Gamma(w,a+b)\ \ge\ -\tfrac{\delta}{32}\bigl(|a|^{2}+|b|^{2}\bigr)-16\delta|w|^{2}\ \ge\ -\tfrac{\delta}{32}\bigl(|a|^{2}+|b|^{2}\bigr)-64\alpha^{2}\cdot\delta\bigl(h(x)+h(y)+1\bigr).

(iv) By the first fact about Γ\Gamma, 0≤Γ(a,a)0\le\Gamma(a,a) and Γ(b,b)≤∣b∣2\Gamma(b,b)\le|b|^{2}, and δ2≤δ\delta^{2}\le\delta since 0<δ<10<\delta<1; so

δ22(Γ(a,a)−Γ(b,b))+δ(∣a∣2+∣b∣2) ≥ δ∣a∣2+(δ−δ22)∣b∣2 ≥ δ2(∣a∣2+∣b∣2).\tfrac{\delta^{2}}{2}\bigl(\Gamma(a,a)-\Gamma(b,b)\bigr)+\delta\bigl(|a|^{2}+|b|^{2}\bigr)\ \ge\ \delta|a|^{2}+\bigl(\delta-\tfrac{\delta^{2}}{2}\bigr)|b|^{2}\ \ge\ \tfrac{\delta}{2}\bigl(|a|^{2}+|b|^{2}\bigr).

(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. The first summand is nonnegative by Monotone, AA-Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §monotone and 0<α0<\alpha. 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}, so, 1α\tfrac{1}{\alpha} being positive and ℓ\ell nonnegative,

⟨Φ(x)−Φ(y),w⟩≥−ℓ α∣x−y∣2≥−ℓ τ.\langle\Phi(x)-\Phi(y),w\rangle\ge-\ell\,\alpha|x-y|^{2}\ge-\ell\,\tau .

(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). The first summand is nonnegative by Monotone, AA-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∣≥−14∣a∣2−∣L(x)∣2\langle L(x),a\rangle\ge-|L(x)|\,|a|\ge-\tfrac{1}{4}|a|^{2}-|L(x)|^{2}, while the third elementary fact, the Lipschitz bound and ∣x∣≤∣x∣V|x|\le|x|_{V} give

∣L(x)∣2≤(cL+ℓ∣x∣)2≤2cL2+2ℓ2∣x∣2≤2cL2+2ℓ2∣x∣V2=2cL2+4ℓ2h(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),

and likewise for yy. Hence

δ(⟨Φ(x),a⟩+⟨Φ(y),b⟩) ≥ −δ4(∣a∣2+∣b∣2)−δ(4cL2+4ℓ2(h(x)+h(y))) ≥ −δ4(∣a∣2+∣b∣2)−(4cL2+4ℓ2) 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),

the last step because 1≤h(x)+h(y)+11\le h(x)+h(y)+1 and h(x)+h(y)≤h(x)+h(y)+1h(x)+h(y)\le h(x)+h(y)+1 and the coefficients are nonnegative.

(vii) We bound the sixth and the tenth group together. Write t=∣x−y∣Vt=|x-y|_{V}, so that their sum is αt2−(g(x)−g(y))\alpha t^{2}-\bigl(g(x)-g(y)\bigr) by (ii). Since x,y∈D(A)⊆Vx,y\in D(A)\subseteq V, the hypotheses on gg give g(x)−g(y)≤∣g(x)−g(y)∣≤ωg(t)g(x)-g(y)\le|g(x)-g(y)|\le\omega_{g}(t), by claim 3 of Properties of the Absolute Value in an Ordered Field, and ∣g(x)−g(y)∣≤∣g(x)∣+∣g(y)∣≤2Cg|g(x)-g(y)|\le|g(x)|+|g(y)|\le2C_{g}, by claims 2 and 5 of that lemma; so g(x)−g(y)g(x)-g(y) is at most both ωg(t)\omega_{g}(t) and 2Cg2C_{g} and therefore

g(x)−g(y)≤ωˉg(t)g(x)-g(y)\le\bar{\omega}_{g}(t)

by The Nondecreasing Envelope of a Truncated Modulus of Continuity §majorant. Note that αt2\alpha t^{2} is nonnegative, being a product of the positive α\alpha with a square, and that 0≤ωg∗(τ)0\le\omega_{g}^{\ast}(\tau), ωg∗\omega_{g}^{\ast} being a modulus of continuity.

Suppose first that 2Cg≤αt22C_{g}\le\alpha t^{2}. Since ωˉg(t)≤2Cg\bar{\omega}_{g}(t)\le2C_{g} by The Nondecreasing Envelope of a Truncated Modulus of Continuity §modulus, transitivity gives g(x)−g(y)≤αt2g(x)-g(y)\le\alpha t^{2}, so αt2−(g(x)−g(y))\alpha t^{2}-(g(x)-g(y)) is nonnegative and hence at least −ωg∗(τ)-\omega_{g}^{\ast}(\tau).

Suppose instead that αt2<2Cg\alpha t^{2}<2C_{g}. Multiplying by the positive 1α\tfrac{1}{\alpha} gives t2<2Cg1αt^{2}<2C_{g}\tfrac{1}{\alpha}, while 1α≤τ\tfrac{1}{\alpha}\le\tau, the difference being the nonnegative α∣x−y∣2\alpha|x-y|^{2}, and 0≤2Cg0\le2C_{g} give 2Cg1α≤2Cgτ2C_{g}\tfrac{1}{\alpha}\le2C_{g}\tau by claim 5 of Elementary Arithmetic in an Ordered Field. Hence t2≤2Cgτt^{2}\le2C_{g}\tau, and so ωˉg(t)≤ωg∗(τ)\bar{\omega}_{g}(t)\le\omega_{g}^{\ast}(\tau) by Sums, Nonnegative Multiples, Monotonicity and Quadratic Reparametrisation of Moduli of Continuity §quadratic, the reparametrisation being taken at c=2Cgc=2C_{g}. Discarding the nonnegative αt2\alpha t^{2},

αt2−(g(x)−g(y)) ≥ −ωˉg(t) ≥ −ωg∗(τ).\alpha t^{2}-\bigl(g(x)-g(y)\bigr)\ \ge\ -\bar{\omega}_{g}(t)\ \ge\ -\omega_{g}^{\ast}(\tau).

In either case

⟨a−b,w⟩−(g(x)−g(y)) ≥ −ωg∗(τ).\langle a-b,w\rangle-\bigl(g(x)-g(y)\bigr)\ \ge\ -\omega_{g}^{\ast}(\tau).

(viii) The bounds (i), (i-a), (i-b), (iii), (iv), (v), (vi) and (vii) account for all ten groups of DD, the last of them for the sixth and the tenth together. Adding them, the terms −δ32(∣a∣2+∣b∣2)-\tfrac{\delta}{32}(|a|^{2}+|b|^{2}) of (iii), δ2(∣a∣2+∣b∣2)\tfrac{\delta}{2}(|a|^{2}+|b|^{2}) of (iv) and −δ4(∣a∣2+∣b∣2)-\tfrac{\delta}{4}(|a|^{2}+|b|^{2}) of (vi) combine to the nonnegative 7δ32(∣a∣2+∣b∣2)\tfrac{7\delta}{32}(|a|^{2}+|b|^{2}), and we obtain

D ≥ −ωg∗(τ)−ℓ τ−(64α2+4cL2+4ℓ2+ν σ(f)) δ(h(x)+h(y)+1).D\ \ge\ -\omega_{g}^{\ast}(\tau)-\ell\,\tau-\bigl(64\alpha^{2}+4c_{L}^{2}+4\ell^{2}+\nu\,\sigma(f)\bigr)\,\delta\bigl(h(x)+h(y)+1\bigr).

Since 1<α1<\alpha we have 1<α21<\alpha^{2}, and as 4cL2+4ℓ24c_{L}^{2}+4\ell^{2} is nonnegative, 64α2+4cL2+4ℓ2≤64α2+(4cL2+4ℓ2)α2=Kα264\alpha^{2}+4c_{L}^{2}+4\ell^{2}\le64\alpha^{2}+(4c_{L}^{2}+4\ell^{2})\alpha^{2}=K\alpha^{2}, so the coefficient above is at most Kα2+ν σ(f)K\alpha^{2}+\nu\,\sigma(f) and the right-hand side is at least −ω1(τ)−ω2(δ(h(x)+h(y)+1),α)-\omega_{1}(\tau)-\omega_{2}(\delta(h(x)+h(y)+1),\alpha). This is the inequality required by The Second-Order Structure Condition for an Equation Operator on a Hilbert Triple §pair, whose displayed hypothesis is imposed only for pairs admitted at α\alpha, as assumed here; so (ω1,ω2)(\omega_{1},\omega_{2}) is a second-order structure pair for FF at RR, and as RR was an arbitrary positive real, FF satisfies the second-order structure condition by The Second-Order Structure Condition for an Equation Operator on a Hilbert Triple §structure.

Claim 4. Let (ek)k∈N(e_{k})_{k\in\mathbb{N}} be an orthonormal basis of HH with ek∈Ve_{k}\in V for every k∈Nk\in\mathbb{N}, and let (Nm)m∈N(N_{m})_{m\in\mathbb{N}} be its sequence of tail forms, as in The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple §tail-forms. Let β,R,ρ∈R\beta,R,\rho\in\mathbb{R} be positive and let δ∈R\delta\in\mathbb{R} satisfy 0<δ<10<\delta<1.

By Elementary Properties of the Trace of a Form along a Square-Summable Sequence §tail the sequence (Trf(Nm∣V))m∈N(\mathrm{Tr}_{f}(N_{m}|_{V}))_{m\in\mathbb{N}} converges to 00, so by claim 3 of Arithmetic of Limits of Real Sequences the sequence with mm-th term νβ2Trf(Nm∣V)\tfrac{\nu\beta}{2}\mathrm{Tr}_{f}(N_{m}|_{V}) converges to 00 as well; since its terms are nonnegative, νβ2\tfrac{\nu\beta}{2} and Trf(Nm∣V)\mathrm{Tr}_{f}(N_{m}|_{V}) being so, there is m0∈Nm_{0}\in\mathbb{N} with

νβ2 Trf(Nm∣V)≤ρfor every m∈N with m0≤m.\tfrac{\nu\beta}{2}\,\mathrm{Tr}_{f}\bigl(N_{m}|_{V}\bigr)\le\rho\qquad\text{for every }m\in\mathbb{N}\text{ with }m_{0}\le m .

Let m∈Nm\in\mathbb{N} satisfy m0≤mm_{0}\le m, and let x∈D(A)x\in D(A), r∈Rr\in\mathbb{R}, p∈Hp\in H and X∈Sym(H)X\in\mathrm{Sym}(H). By claim 10 of Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity we have (X+βNm)∣V=X∣V+β Nm∣V(X+\beta N_{m})|_{V}=X|_{V}+\beta\,N_{m}|_{V} and (X−βNm)∣V=X∣V−β Nm∣V(X-\beta N_{m})|_{V}=X|_{V}-\beta\,N_{m}|_{V}, so Elementary Properties of the Trace of a Form along a Square-Summable Sequence §linear gives

\mathrm{Tr}_{f}\bigl((X+\beta N_{m})|_{V}\bigr)=\mathrm{Tr}_{f}(X|_{V})+\beta\,\mathrm{Tr}_{f}\bigl(N_{m}|_{V}\bigr), \qquad \mathrm{Tr}_{f}\bigl((X-\beta N_{m})|_{V}\bigr)=\mathrm{Tr}_{f}(X|_{V})-\beta\,\mathrm{Tr}_{f}\bigl(N_{m}|_{V}\bigr). $$ Every term of the two shifts other than the trace term is independent of the fourth argument, so, using the shift formulas and the trace identities recorded above,

F^{-}{\delta}(x,r,p,X)-F^{-}{\delta}\bigl(x,r,p,X+\beta N_{m}\bigr)=\tfrac{\nu\beta}{2},\mathrm{Tr}{f}\bigl(N{m}|_{V}\bigr)\le\rho,

F^{+}{\delta}\bigl(x,r,p,X-\beta N{m}\bigr)-F^{+}{\delta}(x,r,p,X)=\tfrac{\nu\beta}{2},\mathrm{Tr}{f}\bigl(N_{m}|_{V}\bigr)\le\rho .

These hold for all such data, in particular for the terms of any sequences as in [The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple §lower](/theorems/7a1fad52-e5e9-4b06-b9f7-3404ec390a28?v=60a64940-3e71-4244-88de-b6da3ae47192#clause-lower) and [The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple §upper](/theorems/7a1fad52-e5e9-4b06-b9f7-3404ec390a28?v=60a64940-3e71-4244-88de-b6da3ae47192#clause-upper), whose $R$-boundedness hypothesis is not needed; rearranged, they are the two inequalities required there. Hence $F$ is tail-insensitive along $(e_{k})_{k\in\mathbb{N}}$. If moreover $H$ is not finite-dimensional as a vector space over $\mathbb{R}$, such a basis exists by [An Orthonormal Basis of the Ambient Space Contained in the Form Space of a Hilbert Triple §basis](/theorems/708f4661-d0e5-4c89-84a3-f4ac1b404da7?v=f8b276c1-f241-4fc2-873e-fe11923c2357#clause-basis), and $F$ then satisfies the tail-insensitivity condition by [The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple §condition](/theorems/7a1fad52-e5e9-4b06-b9f7-3404ec390a28?v=60a64940-3e71-4244-88de-b6da3ae47192#clause-condition). **Claim 5, a bound on the form operator over the admissible sets.** Let $\delta,R\in\mathbb{R}$ satisfy $0<\delta<1$ and $0<R$. Let $\rho$ be the nonnegative real with $\rho^{2}=2R$, given by [Existence and Uniqueness of the Nonnegative Square Root](/theorems/7f783996-7e13-4f8a-9353-21a467864e85?v=9fba8150-5ca0-4dd5-911f-aa0f5cf5feec). If $(z,r,p,X)\in\mathcal{W}$ is [$R$-bounded](/theorems/4640aebc-d86c-4e8f-8b51-dbba74a2d2be?v=5d4402f9-29f2-408b-9701-41c882b2060b#clause-bounded) then $h(z)<R$, so $|z|_{V}^{2}=2h(z)<\rho^{2}$ and therefore $|z|_{V}\le\rho$ by claim 1 of [Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field](/theorems/c4e16e3c-4449-4681-953c-02ad68f9842b?v=d3a024bb-6971-4912-9ff5-7923ca2a4893) and trichotomy, and $|z|\le\rho$. Let $\beta_{0}$ be a bound for $B$ on the set of $\zeta\in V$ with $|\zeta|_{V}\le\rho$, as provided by [Monotone, $A$-Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §bounded](/theorems/ffd56497-3c4f-4c81-8443-c7c97b91b400?v=fae9a4a6-fde1-4289-920d-00ad75746aea#clause-bounded), put $\mu=c_{L}+\ell\rho$ and $N=\beta_{0}+\mu$; then $|\Phi(z)|\le N$ for every such $z$, by [The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle](/theorems/0c7d58a7-82ab-48c0-a8be-ad7b9e2297fc?v=237d76f6-5e7b-450e-974e-4bf327ff854e#clause-triangle) and the bound on $|L|$. We first bound the trace terms. If $(z,r,p,X)$ is $R$-bounded then $\lVert X\rVert<R$, so [Elementary Properties of the Trace of a Form along a Square-Summable Sequence §restriction](/theorems/d74946b5-13a2-4657-81e2-bf67736f3aa1?v=d0d0bd01-a849-4393-b600-07e56979fdaf#clause-restriction) gives $|\mathrm{Tr}_{f}(X|_{V})|\le R\,\sigma(f)$, while $\delta<1$ and $0\le\sigma(f)$ give $\delta\,\sigma(f)\le\sigma(f)$; with the trace identities recorded above and $0\le\tfrac{\nu}{2}$ this yields, putting $C_{\nu}=\tfrac{\nu}{2}(R+1)\,\sigma(f)$,

-\tfrac{\nu}{2},\mathrm{Tr}{f}\bigl(X|{V}+\delta I_{V}\bigr)\ \ge\ -C_{\nu}, \qquad -\tfrac{\nu}{2},\mathrm{Tr}{f}\bigl(X|{V}-\delta I_{V}\bigr)\ \le\ C_{\nu}.

Let $\xi=(x,r,p,X)$ be $R$-bounded. From the formula for $F^{-}_{\delta}$, using $0\le\tfrac12\Gamma(p+\delta a,p+\delta a)$ by the first fact about $\Gamma$, [The Cauchy-Schwarz Inequality in a Real Inner Product Space](/theorems/75e68dc9-c425-4d4e-afd8-53eba404a50e?v=638ad390-44c9-472a-bccb-9ba6242bb219) with $|p|<R$, the second elementary fact in the form $\langle L(x),a\rangle\ge-\tfrac{1}{4}|a|^{2}-|L(x)|^{2}$ together with $|L(x)|\le\mu$ and $\delta<1$, [Monotone, $A$-Monotone and Locally Bounded Nonlinearities on a Hilbert Triple §a-monotone](/theorems/ffd56497-3c4f-4c81-8443-c7c97b91b400?v=fae9a4a6-fde1-4289-920d-00ad75746aea#clause-a-monotone), $|\Phi(x)|\le N$, $0\le h(x)$, $-R\le r$ and $|g(x)|\le C_{g}$,

F^{-}{\delta}(\xi)\ \ge\ \delta|a|^{2}-R|a|-NR-\tfrac{\delta}{4}|a|^{2}-\mu^{2}-\lambda{0}R-C_{g}-C_{\nu}\ =\ \tfrac{3\delta}{4}|a|^{2}-R|a|-C_{-},

where $C_{-}=NR+\mu^{2}+\lambda_{0}R+C_{g}+C_{\nu}$. Similarly, let $\eta=(y,s,p',X')$ be $R$-bounded. Bounding $\tfrac12\Gamma(p'-\delta b,p'-\delta b)$ by $\tfrac12|p'-\delta b|^{2}$, by the first fact about $\Gamma$, expanding the latter by the first elementary fact and using $|p'|<R$, [The Cauchy-Schwarz Inequality in a Real Inner Product Space](/theorems/75e68dc9-c425-4d4e-afd8-53eba404a50e?v=638ad390-44c9-472a-bccb-9ba6242bb219) and $0<\delta<1$,

\tfrac12\Gamma(p'-\delta b,p'-\delta b)\ \le\ \tfrac{1}{2}R^{2}+\delta R|b|+\tfrac{\delta^{2}}{2}|b|^{2},

while $\langle b+\Phi(y),p'-\delta b\rangle\le R|b|-\delta|b|^{2}+NR+\delta N|b|$ by [The Cauchy-Schwarz Inequality in a Real Inner Product Space](/theorems/75e68dc9-c425-4d4e-afd8-53eba404a50e?v=638ad390-44c9-472a-bccb-9ba6242bb219) and $|\Phi(y)|\le N$. Adding these, and using $s\le R$, $0\le h(y)$, $-g(y)\le C_{g}$, the trace bound above, $\delta<1$ and $\tfrac{\delta^{2}}{2}-\delta\le-\tfrac{\delta}{2}$,

F^{+}{\delta}(\eta)\ \le\ -\tfrac{\delta}{2}|b|^{2}+(2R+N)|b|+C{+},

where $C_{+}=\tfrac{1}{2}R^{2}+NR+\lambda_{0}R+C_{g}+C_{\nu}$. By the second elementary fact, $R|a|\le\tfrac{3\delta}{8}|a|^{2}+\tfrac{2R^{2}}{3\delta}$ and $(2R+N)|b|\le\tfrac{\delta}{4}|b|^{2}+\tfrac{(2R+N)^{2}}{\delta}$. Hence the two displays give

F^{-}{\delta}(\xi)\ \ge\ \tfrac{3\delta}{8}|a|^{2}-E,\qquad F^{+}{\delta}(\eta)\ \le\ -\tfrac{\delta}{4}|b|^{2}+E,

where $E=\tfrac{2R^{2}}{3\delta}+\tfrac{(2R+N)^{2}}{\delta}+C_{-}+C_{+}$; in particular $F^{-}_{\delta}(\xi)\ge-E$ and $F^{+}_{\delta}(\eta)\le E$ for all $R$-bounded $\xi$ and $\eta$. Now let $\xi=(x,r,p,X)\in S^{-}_{\delta,R}$. By [Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets §admissible](/theorems/4640aebc-d86c-4e8f-8b51-dbba74a2d2be?v=5d4402f9-29f2-408b-9701-41c882b2060b#clause-admissible) there is an $R$-bounded $\eta$ with $F^{-}_{\delta}(\xi)-F^{+}_{\delta}(\eta)<R$, so $\tfrac{3\delta}{8}|a|^{2}-E\le F^{-}_{\delta}(\xi)<R+F^{+}_{\delta}(\eta)\le R+E$ and therefore $|a|^{2}<\tfrac{8(R+2E)}{3\delta}$. Similarly, if $\eta=(y,s,p',X')\in S^{+}_{\delta,R}$ there is an $R$-bounded $\xi$ with $F^{-}_{\delta}(\xi)-F^{+}_{\delta}(\eta)<R$, so $-\tfrac{\delta}{4}|b|^{2}+E\ge F^{+}_{\delta}(\eta)>F^{-}_{\delta}(\xi)-R\ge-E-R$ and therefore $|b|^{2}<\tfrac{4(R+2E)}{\delta}$. Let $\Lambda$ be the nonnegative real whose square is the larger of $\tfrac{8(R+2E)}{3\delta}$ and $\tfrac{4(R+2E)}{\delta}$, again by [Existence and Uniqueness of the Nonnegative Square Root](/theorems/7f783996-7e13-4f8a-9353-21a467864e85?v=9fba8150-5ca0-4dd5-911f-aa0f5cf5feec). Then $|Ax|\le\Lambda$ whenever $(x,r,p,X)$ lies in $S^{-}_{\delta,R}$ or in $S^{+}_{\delta,R}$, by claim 1 of [Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field](/theorems/c4e16e3c-4449-4681-953c-02ad68f9842b?v=d3a024bb-6971-4912-9ff5-7923ca2a4893) and trichotomy. **Claim 5, the shift modulus.** Put $c=R+2\Lambda+N+\tfrac{\nu}{2}\,\sigma(f)$ and let $\omega$ be the function on the nonnegative reals with $\omega(t)=c\,t+\tfrac{1}{2}t^{2}$. It is nonnegative there. Given a positive $\varepsilon$, let $\delta_{0}$ be the lesser of $1$ and $\tfrac{\varepsilon}{c+1}$, which is positive; every nonnegative $t\le\delta_{0}$ satisfies $t\le1$, hence $t^{2}\le t$ and $\omega(t)\le(c+1)t\le\varepsilon$. So $\omega$ is a modulus of continuity. It is also nondecreasing on the nonnegative reals: for $0\le s\le t$ we have $c\,s\le c\,t$ by [Linear Moduli of Continuity §monotone](/theorems/206eec08-b1fd-4f5b-a4a1-42fc2a8ddbc8?v=be112d1c-eb90-48ca-9371-16fa3ebca6c7#clause-monotone), and $s^{2}\le t^{2}$ by claim 2 of [Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field](/theorems/c4e16e3c-4449-4681-953c-02ad68f9842b?v=d3a024bb-6971-4912-9ff5-7923ca2a4893), whence $\tfrac{1}{2}s^{2}\le\tfrac{1}{2}t^{2}$ by claim 5 of [Elementary Arithmetic in an Ordered Field](/theorems/fe1c552a-759a-469b-86a4-5207560aefaf?v=63c2af8b-b56f-40d4-bc16-3fb0690235bc); adding the two inequalities by claims 3 and 2 of that lemma gives $\omega(s)\le\omega(t)$. Let $q\in H$ and $Y\in\mathrm{Sym}(H)$. Let $(x,r,p,X)\in S^{-}_{\delta,R}$ and put $P=p+\delta a$, so that $|P|\le R+\delta\Lambda\le R+\Lambda$ by [The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §triangle](/theorems/0c7d58a7-82ab-48c0-a8be-ad7b9e2297fc?v=237d76f6-5e7b-450e-974e-4bf327ff854e#clause-triangle). By the third fact about $\Gamma$, [Elementary Identities in a Real Inner Product Space §bilinear](/theorems/5ce8e666-53b7-4958-beed-be505dcf38ba?v=5bbf7092-58eb-4039-aad3-ddfbf22d02dd#clause-bilinear), [The Cauchy-Schwarz Inequality in a Real Inner Product Space](/theorems/75e68dc9-c425-4d4e-afd8-53eba404a50e?v=638ad390-44c9-472a-bccb-9ba6242bb219), [Elementary Properties of the Trace of a Form along a Square-Summable Sequence §linear](/theorems/d74946b5-13a2-4657-81e2-bf67736f3aa1?v=d0d0bd01-a849-4393-b600-07e56979fdaf#clause-linear) together with claim 10 of [Elementary Properties of Bounded Symmetric Bilinear Forms: Norm, Quadratic Form, Order and Continuity](/theorems/ee1a6501-eb70-41c9-a3ea-2490110e3a3e?v=6894704a-d362-4438-a83d-906109126b6b), and the first two facts about $\Gamma$, which give $\Gamma(P,q)\le|P|\,|q|$ and $\tfrac12\Gamma(q,q)\le\tfrac12|q|^{2}$,

F^{-}{\delta}(x,r,p+q,X+Y)-F^{-}{\delta}(x,r,p,X)=-\tfrac{\nu}{2},\mathrm{Tr}{f}(Y|{V})+\Gamma(P,q)+\tfrac12\Gamma(q,q)+\langle a+\Phi(x),q\rangle\ \le\ \tfrac{\nu}{2},\sigma(f),\lVert Y\rVert+\bigl(|P|+|a|+|\Phi(x)|\bigr)|q|+\tfrac{1}{2}|q|^{2},

the trace term being bounded by [Elementary Properties of the Trace of a Form along a Square-Summable Sequence §restriction](/theorems/d74946b5-13a2-4657-81e2-bf67736f3aa1?v=d0d0bd01-a849-4393-b600-07e56979fdaf#clause-restriction). Write $t=|q|+\lVert Y\rVert$, so that $|q|\le t$ and $\lVert Y\rVert\le t$, both being nonnegative; then $|q|^{2}\le t^{2}$ by claim 2 of [Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field](/theorems/c4e16e3c-4449-4681-953c-02ad68f9842b?v=d3a024bb-6971-4912-9ff5-7923ca2a4893), and $|P|+|a|+|\Phi(x)|\le(R+\Lambda)+\Lambda+N$, so, all the coefficients being nonnegative, the right-hand side is at most $c\,t+\tfrac{1}{2}t^{2}=\omega(|q|+\lVert Y\rVert)$. This is the first requirement of [The Shift-Continuity Condition on Admissible Test Data §modulus](/theorems/d5ee1a2e-5473-4025-b8b8-daa65131c780?v=2618888e-84e7-485a-b732-842dc4ebefe4#clause-modulus). Likewise, for $(y,s,p',X')\in S^{+}_{\delta,R}$, putting $P'=p'-\delta b$,

F^{+}{\delta}(y,s,p'+q,X'+Y)-F^{+}{\delta}(y,s,p',X')=-\tfrac{\nu}{2},\mathrm{Tr}{f}(Y|{V})+\Gamma(P',q)+\tfrac12\Gamma(q,q)+\langle b+\Phi(y),q\rangle\ \ge\ -\tfrac{\nu}{2},\sigma(f),\lVert Y\rVert-\bigl(|P'|+|b|+|\Phi(y)|\bigr)|q|\ \ge\ -\omega(|q|+\lVert Y\rVert),

where $\Gamma(P',q)\ge-|P'|\,|q|$ by the second fact about $\Gamma$, and $\tfrac12\Gamma(q,q)$ was discarded as nonnegative by the first. This is the second requirement. Hence $\omega$ is a shift modulus for $F$ at $(\delta,R)$, and as $\delta$ and $R$ were arbitrary, $F$ satisfies the shift-continuity condition by [The Shift-Continuity Condition on Admissible Test Data §continuity](/theorems/d5ee1a2e-5473-4025-b8b8-daa65131c780?v=2618888e-84e7-485a-b732-842dc4ebefe4#clause-continuity). **Claim 6.** Here $H$ is assumed not finite-dimensional. By claims 1, 2, 3, 4 and 5 the operator $F$ is a second-order equation operator on $H$ that is degenerate elliptic and locally strictly proper and satisfies the second-order structure condition, the tail-insensitivity condition and the shift-continuity condition, which are the hypotheses of [A Comparison Principle on a Hilbert Triple under the Second-Order Structure Condition §comparison](/theorems/39ba1c43-8484-4f3f-baee-579cdf02184e?v=877e17f8-b7fc-488b-a750-38cd723ba627#clause-comparison); applying that theorem to $u$, $v$ and $C$ gives $u(x)\le v(x)$ for every $x\in V$.

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