TheoremBase

By contradiction: if comparison fails on nearby points, a penalised doubled function of the two envelopes is perturbed linearly to have a sequentially strict maximum, the parameters are tuned so that every modulus appearing in the second-order test-datum estimate is small, and the estimate then contradicts the assumed positive gap.

Proof

Each result cited is universally quantified over the data in its own statement. Replacing CC by ∣C∣|C| if necessary, we may assume 0≤C0\le C: indeed u(x)≤C≤∣C∣u(x)\le C\le|C| and −∣C∣≤−C≤v(x)-|C|\le-C\le v(x) for every x∈Hx\in H.

Notation. Let J={δ∈R:0<δ<1}J=\{\delta\in\mathbb{R}:0<\delta<1\}. For δ∈J\delta\in J the δ\delta-envelopes uδ−u^{-}_{\delta} and vδ+v^{+}_{\delta} are defined on VV, and by Basic Properties of the δ\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity (iv)

uδ−(x)≤C−δh(x)≤C−δ2∣x∣H2,−vδ+(y)≤C−δh(y)≤C−δ2∣y∣H2(x,y∈V),(i)u^{-}_{\delta}(x)\le C-\delta h(x)\le C-\tfrac{\delta}{2}|x|_{H}^{2},\qquad -v^{+}_{\delta}(y)\le C-\delta h(y)\le C-\tfrac{\delta}{2}|y|_{H}^{2}\qquad(x,y\in V), \tag{i}

and by Basic Properties of the δ\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity (iii) both uδ−u^{-}_{\delta} and −vδ+-v^{+}_{\delta} have closed superlevel sets in HH. The set VV is nonempty, since D(A)∩HD(A)\cap H is dense in 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 (v); fix x∗∈Vx_{*}\in V.

For δ∈J\delta\in J and real α>1\alpha>1 let Φδ,α:V×V→R\Phi_{\delta,\alpha}:V\times V\to\mathbb{R} be given by

Φδ,α(x,y)=uδ−(x)−vδ+(y)−α2∣x−y∣H2.\Phi_{\delta,\alpha}(x,y)=u^{-}_{\delta}(x)-v^{+}_{\delta}(y)-\tfrac{\alpha}{2}|x-y|_{H}^{2}.

By (i) and Closed Superlevel Sets of a Sum on a Product Space and of a Doubled Function (ii), applied with u1=uδ−u_{1}=u^{-}_{\delta}, u2=−vδ+u_{2}=-v^{+}_{\delta}, C1=C2=CC_{1}=C_{2}=C and κ=δ2\kappa=\tfrac{\delta}{2}, the function Φδ,α\Phi_{\delta,\alpha} has closed superlevel sets in H×HH\times H and

Φδ,α(x,y)≤2C−δ2∣(x,y)∣2for all (x,y)∈V×V.(ii)\Phi_{\delta,\alpha}(x,y)\le 2C-\tfrac{\delta}{2}|(x,y)|^{2}\qquad\text{for all }(x,y)\in V\times V. \tag{ii}

Let M(δ,α)M(\delta,\alpha) be the supremum of the values of Φδ,α\Phi_{\delta,\alpha}, and let N(α)N(\alpha) be the supremum of the set of all numbers Φδ,α(x,y)\Phi_{\delta,\alpha}(x,y) with δ∈J\delta\in J and (x,y)∈V×V(x,y)\in V\times V. Both are real numbers, and the needed properties come from Penalised Suprema: Monotonicity, Near-Maximisers, and Vanishing Penalty along a Doubling Sequence: applied with Z=V×VZ=V\times V, ψ(x,y)=uδ−(x)−vδ+(y)\psi(x,y)=u^{-}_{\delta}(x)-v^{+}_{\delta}(y), which is bounded above by 2C2C by (i), D(x,y)=12∣x−y∣H2D(x,y)=\tfrac12|x-y|_{H}^{2} and z0=(x∗,x∗)z_{0}=(x_{*},x_{*}), it gives claims 1 to 3 for the function α↦M(δ,α)\alpha\mapsto M(\delta,\alpha); applied with Z=J×V×VZ=J\times V\times V, ψ(δ,x,y)=uδ−(x)−vδ+(y)\psi(\delta,x,y)=u^{-}_{\delta}(x)-v^{+}_{\delta}(y), D(δ,x,y)=12∣x−y∣H2D(\delta,x,y)=\tfrac12|x-y|_{H}^{2} and z0=(12,x∗,x∗)z_{0}=(\tfrac12,x_{*},x_{*}), it gives claims 1, 2 and 4 for NN. In particular, for every real β0>1\beta_{0}>1, with βk=2kβ0\beta_{k}=2^{k}\beta_{0} for k∈Nk\in\mathbb{N} (so that 1<β0≤βk1<\beta_{0}\le\beta_{k} for every kk, by claims 2 and 5 of Properties of Natural Number Powers in a Field, and N(βk)N(\beta_{k}) is defined),

the sequence whose k-th term is N(βk)−N(βk+1) converges to 0,(iii)\text{the sequence whose }k\text{-th term is }N(\beta_{k})-N(\beta_{k+1})\text{ converges to }0, \tag{iii}

this being claim 4. Moreover M(δ,α)≤N(α)M(\delta,\alpha)\le N(\alpha) for every δ∈J\delta\in J. By Basic Properties of the δ\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity (vii) we have uδ′−(x)+(δ′−δ)h(x)≤uδ−(x)u^{-}_{\delta'}(x)+(\delta'-\delta)h(x)\le u^{-}_{\delta}(x) and vδ+(y)+(δ′−δ)h(y)≤vδ′+(y)v^{+}_{\delta}(y)+(\delta'-\delta)h(y)\le v^{+}_{\delta'}(y) for x,y∈Vx,y\in V whenever δ≤δ′\delta\le\delta' in JJ; adding the first inequality to the second multiplied by −1-1 (claim 3 of Elementary Order Arithmetic in an Ordered Field in its weak form, and claim 4 of that lemma) and then subtracting α2∣x−y∣H2\tfrac{\alpha}{2}|x-y|_{H}^{2} from both sides gives

Φδ′,α(x,y)+(δ′−δ)(h(x)+h(y))≤Φδ,α(x,y)for x,y∈V and δ,δ′∈J with δ≤δ′.(iv′)\Phi_{\delta',\alpha}(x,y)+(\delta'-\delta)\bigl(h(x)+h(y)\bigr)\le\Phi_{\delta,\alpha}(x,y)\qquad\text{for }x,y\in V\text{ and }\delta,\delta'\in J\text{ with }\delta\le\delta'. \tag{iv$'$}

Since 0≤(δ′−δ)(h(x)+h(y))0\le(\delta'-\delta)(h(x)+h(y)) by The Penalty Function h=12∣⋅∣V2h=\tfrac12|\cdot|_V^2 of a Hilbert Triple: Expansion Identities, Closed Sublevel Sets, Density and Local Bounds (i) and claims 2 and 5 of Elementary Arithmetic in an Ordered Field, (iv′') gives Φδ′,α≤Φδ,α\Phi_{\delta',\alpha}\le\Phi_{\delta,\alpha} on V×VV\times V, so

M(δ′,α)≤M(δ,α)for δ,δ′∈J with δ≤δ′.(iv)M(\delta',\alpha)\le M(\delta,\alpha)\qquad\text{for }\delta,\delta'\in J\text{ with }\delta\le\delta'. \tag{iv}

Proof of claim 1. Suppose the claim fails. Then there is a positive ϵ0∈R\epsilon_{0}\in\mathbb{R} such that for every positive θ∈R\theta\in\mathbb{R} there are x,y∈Vx,y\in V with ∣x−y∣H≤θ|x-y|_{H}\le\theta and ϵ0<u(x)−v(y)\epsilon_{0}<u(x)-v(y).

Step 1. ϵ0≤N(α)\epsilon_{0}\le N(\alpha) for every real α>1\alpha>1. Let α>1\alpha>1 and let μ∈R\mu\in\mathbb{R} be positive. Choose a positive θ\theta with α2θ2≤μ2\tfrac{\alpha}{2}\theta^{2}\le\tfrac{\mu}{2} and then x,y∈Vx,y\in V with ∣x−y∣H≤θ|x-y|_{H}\le\theta and ϵ0<u(x)−v(y)\epsilon_{0}<u(x)-v(y). By The Penalty Function h=12∣⋅∣V2h=\tfrac12|\cdot|_V^2 of a Hilbert Triple: Expansion Identities, Closed Sublevel Sets, Density and Local Bounds (i) and claim 2 of Elementary Arithmetic in an Ordered Field the number h(x)+h(y)h(x)+h(y) is nonnegative, so there is δ∈J\delta\in J with δ(h(x)+h(y))≤μ2\delta\bigl(h(x)+h(y)\bigr)\le\tfrac{\mu}{2}: take δ=12\delta=\tfrac12 if h(x)+h(y)=0h(x)+h(y)=0, and otherwise any positive δ\delta below both 12\tfrac12 and μ2(h(x)+h(y))\tfrac{\mu}{2(h(x)+h(y))}. By Basic Properties of the δ\delta-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity (i), u(x)−δh(x)≤uδ−(x)u(x)-\delta h(x)\le u^{-}_{\delta}(x) and vδ+(y)≤v(y)+δh(y)v^{+}_{\delta}(y)\le v(y)+\delta h(y), whence

N(α)≥Φδ,α(x,y)≥u(x)−v(y)−δ(h(x)+h(y))−α2∣x−y∣H2>ϵ0−μ,N(\alpha)\ge\Phi_{\delta,\alpha}(x,y)\ge u(x)-v(y)-\delta\bigl(h(x)+h(y)\bigr)-\tfrac{\alpha}{2}|x-y|_{H}^{2}>\epsilon_{0}-\mu ,

where ∣x−y∣H2≤θ2|x-y|_{H}^{2}\le\theta^{2} by Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. As μ\mu was an arbitrary positive real, Comparison of Real Numbers with Arbitrary Positive Slack (i) gives ϵ0≤N(α)\epsilon_{0}\le N(\alpha).

Step 2 (constants that do not move). Set B=4C+4B=4C+4, so that 0≤C≤B0\le C\le B and 3B+23B+2 is positive. Let λ\lambda be a properness constant for FF at 3B+23B+2 and let (ω1,ω2)(\omega_{1},\omega_{2}) be a second-order structure pair for FF at 3B+23B+2; both exist by hypothesis. By the tail-insensitivity condition fix an orthonormal basis (ek)k∈N(e_{k})_{k\in\mathbb{N}} of HH with ek∈Ve_{k}\in V for every k∈Nk\in\mathbb{N} along which FF is tail-insensitive; this basis is fixed once and for all, before the parameters chosen in the steps below. Set ϵ1=λϵ020\epsilon_{1}=\tfrac{\lambda\epsilon_{0}}{20}, a positive real, and use clause 2 of Modulus of Continuity to choose a positive real τ(1)\tau^{(1)} such that every tt with 0≤t≤τ(1)0\le t\le\tau^{(1)} satisfies ω1(t)≤ϵ1\omega_{1}(t)\le\epsilon_{1}.

Step 3 (the parameters θ\theta and α\alpha). Choose a positive θ∈R\theta\in\mathbb{R} with

θ≤1,8θ≤ϵ0,96θ≤τ(1).\theta\le1,\qquad 8\theta\le\epsilon_{0},\qquad 96\theta\le\tau^{(1)}.

By The Archimedean Property of the Real Numbers choose m0∈Nm_{0}\in\mathbb{N} with 2τ(1)≤m0\tfrac{2}{\tau^{(1)}}\le m_{0} and put m=m0+1m=m_{0}+1, so that m∈Nm\in\mathbb{N}, 2τ(1)≤m\tfrac{2}{\tau^{(1)}}\le m and 2≤m2\le m (as 1≤m01\le m_{0}). For k∈Nk\in\mathbb{N} put βk=2km\beta_{k}=2^{k}m, and let β0\beta_{0} denote mm itself, as in claim 4 of Penalised Suprema: Monotonicity, Near-Maximisers, and Vanishing Penalty along a Doubling Sequence; since 1<2≤m1<2\le m, (iii) applies with β0=m\beta_{0}=m: the sequence whose kk-th term is N(βk)−N(βk+1)N(\beta_{k})-N(\beta_{k+1}) converges to 00. Choose k∈Nk\in\mathbb{N} with N(βk)−N(βk+1)≤θN(\beta_{k})-N(\beta_{k+1})\le\theta and set α=βk+1\alpha=\beta_{k+1}, so that α2=βk\tfrac{\alpha}{2}=\beta_{k}. Since 1≤2k1\le2^{k} and 1≤2k+11\le2^{k+1} by claims 2 and 5 of Properties of Natural Number Powers in a Field, we have 2≤m≤βk=α22\le m\le\beta_{k}=\tfrac{\alpha}{2} and m≤αm\le\alpha; hence 1<α21<\tfrac{\alpha}{2} and 1<α1<\alpha, so that M(δ,α2)M(\delta,\tfrac{\alpha}{2}), M(δ,α)M(\delta,\alpha) and N(α)N(\alpha) are defined, and 2τ(1)≤α\tfrac{2}{\tau^{(1)}}\le\alpha, that is, 1α≤τ(1)2\tfrac{1}{\alpha}\le\tfrac{\tau^{(1)}}{2} (claims 4 and 5 of Elementary Arithmetic in an Ordered Field).

Step 4 (the parameters θ′\theta' and δ\delta). The function t↦ω2(t,α)t\mapsto\omega_{2}(t,\alpha) on the nonnegative reals is a modulus of continuity by The Second-Order Structure Condition for an Equation Operator on a Hilbert Triple (ii), so by clause 2 of Modulus of Continuity there is a positive real τ(2)\tau^{(2)} such that every tt with 0≤t≤τ(2)0\le t\le\tau^{(2)} satisfies ω2(t,α)≤ϵ1\omega_{2}(t,\alpha)\le\epsilon_{1}. Choose a positive θ′∈R\theta'\in\mathbb{R} with

θ′≤θ,16θ′≤τ(2).\theta'\le\theta,\qquad 16\theta'\le\tau^{(2)}.

By the definition of N(α)N(\alpha) as a supremum there are δ1∈J\delta_{1}\in J and (x,y)∈V×V(x,y)\in V\times V with N(α)−θ′<Φδ1,α(x,y)≤M(δ1,α)N(\alpha)-\theta'<\Phi_{\delta_{1},\alpha}(x,y)\le M(\delta_{1},\alpha); by (iv), N(α)−θ′<M(δ,α)N(\alpha)-\theta'<M(\delta,\alpha) for every δ∈J\delta\in J with δ≤δ1\delta\le\delta_{1}. Choose such a δ\delta with in addition 4δ≤τ(2)4\delta\le\tau^{(2)}. By Step 1 and 8θ′≤8θ≤ϵ08\theta'\le8\theta\le\epsilon_{0},

0≤ϵ0−θ′≤N(α)−θ′<M(δ,α).(v)0\le\epsilon_{0}-\theta'\le N(\alpha)-\theta'<M(\delta,\alpha). \tag{v}

Step 5 (the maximum point). Choose (x2,y2)∈V×V(x_{2},y_{2})\in V\times V with M(δ,α)−θ′2≤Φδ,α(x2,y2)M(\delta,\alpha)-\tfrac{\theta'}{2}\le\Phi_{\delta,\alpha}(x_{2},y_{2}). By (ii), (v) and θ′≤1\theta'\le1,

δ2∣(x2,y2)∣2≤2C−Φδ,α(x2,y2)≤2C−M(δ,α)+θ′2≤2C+1,\tfrac{\delta}{2}|(x_{2},y_{2})|^{2}\le2C-\Phi_{\delta,\alpha}(x_{2},y_{2})\le2C-M(\delta,\alpha)+\tfrac{\theta'}{2}\le2C+1,

so ∣(x2,y2)∣≤Γ|(x_{2},y_{2})|\le\Gamma, where Γ\Gamma denotes the nonnegative square root of 4C+2δ\tfrac{4C+2}{\delta}. Let Γ′\Gamma' denote the nonnegative square root of 4δ(2C+12+2Γ+4δ)\tfrac{4}{\delta}\bigl(2C+\tfrac12+2\Gamma+\tfrac{4}{\delta}\bigr), let GG denote the nonnegative square root of 12αθ12\alpha\theta, and set

R=2B+1δ+3B+2+8α+2+G+2α+1,R=\frac{2B+1}{\delta}+3B+2+8\alpha+2+G+2\alpha+1 ,

so that the four inequalities 2B+1δ<R\tfrac{2B+1}{\delta}<R, 3B+2<R3B+2<R, 8α+2<R8\alpha+2<R and G+2α<RG+2\alpha<R hold, all summands being positive. Let ω\omega be a shift modulus for FF at (δ,R)(\delta,R), which exists by hypothesis, and choose a positive τ(0)\tau^{(0)} such that every tt with 0≤t≤τ(0)0\le t\le\tau^{(0)} satisfies ω(t)≤ϵ1\omega(t)\le\epsilon_{1}.

Now choose a positive σ∈R\sigma\in\mathbb{R} with

σ≤1,σ≤τ(0)2,σ (2Γ+2Γ′)≤θ′2.\sigma\le1,\qquad \sigma\le\tfrac{\tau^{(0)}}{2},\qquad \sigma\,(2\Gamma+2\Gamma')\le\tfrac{\theta'}{2}.

The product H×HH\times H is a real Hilbert space by Properties of the Product of Two Real Inner Product Spaces (vi), and V×VV\times V is a nonempty subset of it. By (ii) and A Linear Perturbation Producing a Sequentially Strict Maximum under a Coercive Bound, applied to Φδ,α\Phi_{\delta,\alpha} with the constant 2C2C, the positive number δ2\tfrac{\delta}{2} and the positive number σ\sigma, there are (p,q)∈H×H(p,q)\in H\times H with ∣(p,q)∣≤σ|(p,q)|\le\sigma and (x^,y^)∈V×V(\hat{x},\hat{y})\in V\times V such that the function with value

Φδ,α(x,y)−⟨(p,q),(x,y)⟩=Φδ,α(x,y)−⟨p,x⟩H−⟨q,y⟩H\Phi_{\delta,\alpha}(x,y)-\langle(p,q),(x,y)\rangle=\Phi_{\delta,\alpha}(x,y)-\langle p,x\rangle_{H}-\langle q,y\rangle_{H}

at (x,y)(x,y) attains a sequentially strict maximum on V×VV\times V at (x^,y^)(\hat{x},\hat{y}); the displayed identity is the formula for the inner product of the product in The Product of Two Real Inner Product Spaces (i), and Properties of the Product of Two Real Inner Product Spaces (ii) gives ∣p∣H≤σ|p|_{H}\le\sigma and ∣q∣H≤σ|q|_{H}\le\sigma.

Step 6 (the maximum point nearly maximises Φδ,α\Phi_{\delta,\alpha}). Write ρ=∣(x^,y^)∣\rho=|(\hat{x},\hat{y})|, so that ∣x^∣H+∣y^∣H≤2ρ|\hat{x}|_{H}+|\hat{y}|_{H}\le2\rho and ∣x2∣H+∣y2∣H≤2Γ|x_{2}|_{H}+|y_{2}|_{H}\le2\Gamma. By the maximum property and The Cauchy–Schwarz Inequality in a Real Inner Product Space,

Φδ,α(x^,y^) ≥ Φδ,α(x2,y2)−σ(∣x2∣H+∣y2∣H)−σ(∣x^∣H+∣y^∣H) ≥ M(δ,α)−θ′2−2σΓ−2σρ.(vi)\Phi_{\delta,\alpha}(\hat{x},\hat{y})\ \ge\ \Phi_{\delta,\alpha}(x_{2},y_{2})-\sigma\bigl(|x_{2}|_{H}+|y_{2}|_{H}\bigr)-\sigma\bigl(|\hat{x}|_{H}+|\hat{y}|_{H}\bigr)\ \ge\ M(\delta,\alpha)-\tfrac{\theta'}{2}-2\sigma\Gamma-2\sigma\rho . \tag{vi}

Using σ≤1\sigma\le1, M(δ,α)≥0M(\delta,\alpha)\ge0, θ′≤1\theta'\le1 and (ii),

δ2ρ2≤2C−Φδ,α(x^,y^)≤2C+12+2Γ+2ρ,\tfrac{\delta}{2}\rho^{2}\le2C-\Phi_{\delta,\alpha}(\hat{x},\hat{y})\le2C+\tfrac12+2\Gamma+2\rho ,

and since δ4(ρ−4δ)2≥0\tfrac{\delta}{4}\bigl(\rho-\tfrac{4}{\delta}\bigr)^{2}\ge0 gives 2ρ≤δ4ρ2+4δ2\rho\le\tfrac{\delta}{4}\rho^{2}+\tfrac{4}{\delta}, we obtain δ4ρ2≤2C+12+2Γ+4δ\tfrac{\delta}{4}\rho^{2}\le2C+\tfrac12+2\Gamma+\tfrac{4}{\delta}, that is, ρ≤Γ′\rho\le\Gamma'. Substituting ρ≤Γ′\rho\le\Gamma' into (vi) and using σ(2Γ+2Γ′)≤θ′2\sigma(2\Gamma+2\Gamma')\le\tfrac{\theta'}{2},

M(δ,α)−θ′ ≤ Φδ,α(x^,y^).(vii)M(\delta,\alpha)-\theta'\ \le\ \Phi_{\delta,\alpha}(\hat{x},\hat{y}). \tag{vii}

Step 7 (the bounds required by the estimate). Since α2∣x^−y^∣H2≥0\tfrac{\alpha}{2}|\hat{x}-\hat{y}|_{H}^{2}\ge0, (vii), (v), θ′≤θ\theta'\le\theta and 8θ≤ϵ08\theta\le\epsilon_{0} give

uδ−(x^)−vδ+(y^) ≥ Φδ,α(x^,y^) ≥ M(δ,α)−θ′ ≥ ϵ0−2θ′ ≥ ϵ0−2θ ≥ 34ϵ0 > 0.(viii)u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\ \ge\ \Phi_{\delta,\alpha}(\hat{x},\hat{y})\ \ge\ M(\delta,\alpha)-\theta'\ \ge\ \epsilon_{0}-2\theta'\ \ge\ \epsilon_{0}-2\theta\ \ge\ \tfrac{3}{4}\epsilon_{0}\ >\ 0. \tag{viii}

By (i) we have uδ−(x^)≤Cu^{-}_{\delta}(\hat{x})\le C and −C≤vδ+(y^)-C\le v^{+}_{\delta}(\hat{y}); combined with (viii) this yields uδ−(x^)≥vδ+(y^)≥−Cu^{-}_{\delta}(\hat{x})\ge v^{+}_{\delta}(\hat{y})\ge-C and vδ+(y^)≤uδ−(x^)≤Cv^{+}_{\delta}(\hat{y})\le u^{-}_{\delta}(\hat{x})\le C, so

∣uδ−(x^)∣≤C≤B,∣vδ+(y^)∣≤C≤B.|u^{-}_{\delta}(\hat{x})|\le C\le B,\qquad |v^{+}_{\delta}(\hat{y})|\le C\le B .

By (i) again, δh(x^)≤C−uδ−(x^)≤2C≤B\delta h(\hat{x})\le C-u^{-}_{\delta}(\hat{x})\le2C\le B and δh(y^)≤vδ+(y^)+C≤2C≤B\delta h(\hat{y})\le v^{+}_{\delta}(\hat{y})+C\le2C\le B.

By (vii) the point (x^,y^)(\hat{x},\hat{y}) satisfies the hypothesis of Penalised Suprema: Monotonicity, Near-Maximisers, and Vanishing Penalty along a Doubling Sequence (iii) for the function α↦M(δ,α)\alpha\mapsto M(\delta,\alpha) with the parameter α\alpha and the number θ′\theta', so

α4∣x^−y^∣H2=α2⋅12∣x^−y^∣H2≤M(δ,α2)−M(δ,α)+θ′≤N(βk)−(N(βk+1)−θ′)+θ′≤θ+2θ′≤3θ,\tfrac{\alpha}{4}|\hat{x}-\hat{y}|_{H}^{2}=\tfrac{\alpha}{2}\cdot\tfrac12|\hat{x}-\hat{y}|_{H}^{2}\le M\bigl(\delta,\tfrac{\alpha}{2}\bigr)-M(\delta,\alpha)+\theta'\le N(\beta_{k})-\bigl(N(\beta_{k+1})-\theta'\bigr)+\theta'\le\theta+2\theta'\le3\theta ,

using α2=βk\tfrac{\alpha}{2}=\beta_{k}, M(δ,βk)≤N(βk)M(\delta,\beta_{k})\le N(\beta_{k}), Step 4, Step 3 and θ′≤θ\theta'\le\theta. Hence

α∣x^−y^∣H2≤12θ,α∣x^−y^∣H=α⋅α∣x^−y^∣H2≤G,(ix)\alpha|\hat{x}-\hat{y}|_{H}^{2}\le12\theta,\qquad \alpha|\hat{x}-\hat{y}|_{H}=\sqrt{\alpha\cdot\alpha|\hat{x}-\hat{y}|_{H}^{2}}\le G , \tag{ix}

where square roots are compared by Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field.

Step 8 (the contradiction). Choose a positive ε∈R\varepsilon\in\mathbb{R} with

ε≤1,(2α+1)ε≤τ(0)2,32αε2≤τ(1),(4+4G)ε≤τ(2)4,16αε2≤τ(2),2λε+2ε≤ϵ1.\varepsilon\le1,\qquad (2\alpha+1)\varepsilon\le\tfrac{\tau^{(0)}}{2},\qquad 32\alpha\varepsilon^{2}\le\tau^{(1)},\qquad (4+4G)\varepsilon\le\tfrac{\tau^{(2)}}{4},\qquad 16\alpha\varepsilon^{2}\le\tau^{(2)},\qquad 2\lambda\varepsilon+2\varepsilon\le\epsilon_{1}.

All the hypotheses of The Second-Order Test-Datum Estimate at a Sequentially Strict Maximum of the Doubled Function now hold for the data δ,α,σ,ε,B,G,R\delta,\alpha,\sigma,\varepsilon,B,G,R, the vectors p,qp,q, the point (x^,y^)(\hat{x},\hat{y}), the basis (ek)k∈N(e_{k})_{k\in\mathbb{N}}, the constant λ\lambda, the pair (ω1,ω2)(\omega_{1},\omega_{2}) and the modulus ω\omega, by Steps 2 to 7. It provides x1,y1∈D(A)x_{1},y_{1}\in D(A) and nonnegative τ1,τ2\tau_{1},\tau_{2} with ∣x1−x^∣H<ε|x_{1}-\hat{x}|_{H}<\varepsilon, ∣y1−y^∣H<ε|y_{1}-\hat{y}|_{H}<\varepsilon, ∣uδ−(x1)−uδ−(x^)∣<ε|u^{-}_{\delta}(x_{1})-u^{-}_{\delta}(\hat{x})|<\varepsilon, ∣vδ+(y1)−vδ+(y^)∣<ε|v^{+}_{\delta}(y_{1})-v^{+}_{\delta}(\hat{y})|<\varepsilon, τ1≤(2α+1)ε+σ≤τ(0)\tau_{1}\le(2\alpha+1)\varepsilon+\sigma\le\tau^{(0)}, τ2≤τ(0)\tau_{2}\le\tau^{(0)} and the estimate of The Second-Order Test-Datum Estimate at a Sequentially Strict Maximum of the Doubled Function (i).

The first modulus. Write t=∣x1−y1∣Ht=|x_{1}-y_{1}|_{H} and ρ0=∣x^−y^∣H\rho_{0}=|\hat{x}-\hat{y}|_{H}. By The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity (i), t≤∣x1−x^∣H+ρ0+∣y^−y1∣H≤ρ0+2εt\le|x_{1}-\hat{x}|_{H}+\rho_{0}+|\hat{y}-y_{1}|_{H}\le\rho_{0}+2\varepsilon, so t2≤(ρ0+2ε)2t^{2}\le(\rho_{0}+2\varepsilon)^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. Since (a+b)2≤2a2+2b2(a+b)^{2}\le2a^{2}+2b^{2} for all real a,ba,b, because 2a2+2b2−(a+b)2=(a−b)2≥02a^{2}+2b^{2}-(a+b)^{2}=(a-b)^{2}\ge0, we get

αt2≤2αρ02+8αε2≤24θ+τ(1)4≤τ(1)4+τ(1)4=τ(1)2,\alpha t^{2}\le2\alpha\rho_{0}^{2}+8\alpha\varepsilon^{2}\le24\theta+\tfrac{\tau^{(1)}}{4}\le\tfrac{\tau^{(1)}}{4}+\tfrac{\tau^{(1)}}{4}=\tfrac{\tau^{(1)}}{2},

using (ix), 32αε2≤τ(1)32\alpha\varepsilon^{2}\le\tau^{(1)} and 96θ≤τ(1)96\theta\le\tau^{(1)}; together with 1α≤τ(1)2\tfrac{1}{\alpha}\le\tfrac{\tau^{(1)}}{2} from Step 3 this gives 0≤αt2+1α≤τ(1)0\le\alpha t^{2}+\tfrac{1}{\alpha}\le\tau^{(1)}, hence ω1(αt2+1α)≤ϵ1\omega_{1}\bigl(\alpha t^{2}+\tfrac{1}{\alpha}\bigr)\le\epsilon_{1} by Step 2.

The penalty at the test points. Since δ2∈J\tfrac{\delta}{2}\in J and δ2≤δ\tfrac{\delta}{2}\le\delta, (iv′') applied with δ2\tfrac{\delta}{2} and δ\delta in the roles of δ\delta and δ′\delta' gives

Φδ,α(x1,y1)+δ2(h(x1)+h(y1))≤Φδ/2,α(x1,y1)≤M(δ2,α)≤N(α).(x)\Phi_{\delta,\alpha}(x_{1},y_{1})+\tfrac{\delta}{2}\bigl(h(x_{1})+h(y_{1})\bigr)\le\Phi_{\delta/2,\alpha}(x_{1},y_{1})\le M\bigl(\tfrac{\delta}{2},\alpha\bigr)\le N(\alpha). \tag{x}

On the other hand, claim 9 of Properties of the Absolute Value in an Ordered Field turns the two envelope inequalities provided by the estimate into uδ−(x1)>uδ−(x^)−εu^{-}_{\delta}(x_{1})>u^{-}_{\delta}(\hat{x})-\varepsilon and vδ+(y1)<vδ+(y^)+εv^{+}_{\delta}(y_{1})<v^{+}_{\delta}(\hat{y})+\varepsilon, while expanding the square and using (ix) and αρ0≤G\alpha\rho_{0}\le G,

α2t2≤α2(ρ0+2ε)2=α2ρ02+2ε αρ0+2αε2≤α2ρ02+2Gε+2αε2.\tfrac{\alpha}{2}t^{2}\le\tfrac{\alpha}{2}(\rho_{0}+2\varepsilon)^{2}=\tfrac{\alpha}{2}\rho_{0}^{2}+2\varepsilon\,\alpha\rho_{0}+2\alpha\varepsilon^{2}\le\tfrac{\alpha}{2}\rho_{0}^{2}+2G\varepsilon+2\alpha\varepsilon^{2}.

Hence, by (vii),

Φδ,α(x1,y1) ≥ uδ−(x^)−vδ+(y^)−α2ρ02−2ε−2Gε−2αε2 = Φδ,α(x^,y^)−(2+2G)ε−2αε2 ≥ M(δ,α)−θ′−(2+2G)ε−2αε2.\Phi_{\delta,\alpha}(x_{1},y_{1})\ \ge\ u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})-\tfrac{\alpha}{2}\rho_{0}^{2}-2\varepsilon-2G\varepsilon-2\alpha\varepsilon^{2}\ =\ \Phi_{\delta,\alpha}(\hat{x},\hat{y})-(2+2G)\varepsilon-2\alpha\varepsilon^{2}\ \ge\ M(\delta,\alpha)-\theta'-(2+2G)\varepsilon-2\alpha\varepsilon^{2}.

Combining this with (x) and with N(α)−θ′<M(δ,α)N(\alpha)-\theta'<M(\delta,\alpha) from Step 4,

δ2(h(x1)+h(y1))≤N(α)−M(δ,α)+θ′+(2+2G)ε+2αε2≤2θ′+(2+2G)ε+2αε2,\tfrac{\delta}{2}\bigl(h(x_{1})+h(y_{1})\bigr)\le N(\alpha)-M(\delta,\alpha)+\theta'+(2+2G)\varepsilon+2\alpha\varepsilon^{2}\le2\theta'+(2+2G)\varepsilon+2\alpha\varepsilon^{2},

and therefore, by 16θ′≤τ(2)16\theta'\le\tau^{(2)}, (4+4G)ε≤τ(2)4(4+4G)\varepsilon\le\tfrac{\tau^{(2)}}{4}, 16αε2≤τ(2)16\alpha\varepsilon^{2}\le\tau^{(2)} and 4δ≤τ(2)4\delta\le\tau^{(2)},

δ(h(x1)+h(y1)+1)≤4θ′+(4+4G)ε+4αε2+δ≤τ(2)4+τ(2)4+τ(2)4+τ(2)4=τ(2).\delta\bigl(h(x_{1})+h(y_{1})+1\bigr)\le4\theta'+(4+4G)\varepsilon+4\alpha\varepsilon^{2}+\delta\le\tfrac{\tau^{(2)}}{4}+\tfrac{\tau^{(2)}}{4}+\tfrac{\tau^{(2)}}{4}+\tfrac{\tau^{(2)}}{4}=\tau^{(2)} .

The left-hand side is nonnegative by The Penalty Function h=12∣⋅∣V2h=\tfrac12|\cdot|_V^2 of a Hilbert Triple: Expansion Identities, Closed Sublevel Sets, Density and Local Bounds (i), so ω2(δ(h(x1)+h(y1)+1),α)≤ϵ1\omega_{2}\bigl(\delta(h(x_{1})+h(y_{1})+1),\alpha\bigr)\le\epsilon_{1} by the choice of τ(2)\tau^{(2)} in Step 4.

Conclusion. Each of ω(τ1)\omega(\tau_{1}), ω(τ2)\omega(\tau_{2}), ω1(αt2+1α)\omega_{1}\bigl(\alpha t^{2}+\tfrac{1}{\alpha}\bigr) and ω2(δ(h(x1)+h(y1)+1),α)\omega_{2}\bigl(\delta(h(x_{1})+h(y_{1})+1),\alpha\bigr) is at most ϵ1\epsilon_{1}, and 2λε+2ε≤ϵ12\lambda\varepsilon+2\varepsilon\le\epsilon_{1}, so the estimate gives

λ(uδ−(x^)−vδ+(y^))≤5ϵ1=λϵ04.\lambda\bigl(u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\bigr)\le5\epsilon_{1}=\tfrac{\lambda\epsilon_{0}}{4}.

On the other hand (viii) and λ>0\lambda>0 give λ(uδ−(x^)−vδ+(y^))≥34λϵ0\lambda\bigl(u^{-}_{\delta}(\hat{x})-v^{+}_{\delta}(\hat{y})\bigr)\ge\tfrac{3}{4}\lambda\epsilon_{0}. Dividing by the positive number λϵ0\lambda\epsilon_{0} yields 34≤14\tfrac{3}{4}\le\tfrac{1}{4}, which is false. This contradiction proves claim 1.

Proof of claim 2. Let x∈Vx\in V and let ϵ∈R\epsilon\in\mathbb{R} be positive. By claim 1 there is a positive θ\theta such that all x′,y′∈Vx',y'\in V with ∣x′−y′∣H≤θ|x'-y'|_{H}\le\theta satisfy u(x′)−v(y′)≤ϵu(x')-v(y')\le\epsilon; taking x′=y′=xx'=y'=x, which is legitimate because ∣x−x∣H=0≤θ|x-x|_{H}=0\le\theta, gives u(x)−v(x)≤ϵu(x)-v(x)\le\epsilon. As ϵ\epsilon was an arbitrary positive real, Comparison of Real Numbers with Arbitrary Positive Slack (i) gives u(x)−v(x)≤0u(x)-v(x)\le0, that is, u(x)≤v(x)u(x)\le v(x).

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