TheoremBase

The second-order structure inequality is required for fewer pairs of forms than the first-order one, and a first-order operator has shifts that ignore the form argument, so both tail differences vanish identically.

Proof

Each result cited is universally quantified over the data in its own statement.

Proof of claim 1. Let R∈RR\in\mathbb{R} be positive and let (Ο‰1,Ο‰2)(\omega_{1},\omega_{2}) be a structure pair for FF at RR. The requirements that The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple (i) and The Second-Order Structure Condition for an Equation Operator on a Hilbert Triple (ii) place on Ο‰1\omega_{1} and on Ο‰2\omega_{2} are the same, namely that Ο‰1\omega_{1} be a modulus of continuity and that Ο‰2\omega_{2} be a real-valued function on the pairs (t,Ξ±)(t,\alpha) with 0≀t0\le t and 1<Ξ±1<\alpha for which t↦ω2(t,Ξ±)t\mapsto\omega_{2}(t,\alpha) is a modulus of continuity for each real Ξ±>1\alpha>1; and the displayed inequality is the same in the two clauses. The two clauses differ only in the range of the form arguments: the first demands the inequality for all X,Y∈Sym(H)X,Y\in\mathrm{Sym}(H), the second only for the pairs (X,Y)(X,Y) of members of Sym(H)\mathrm{Sym}(H) that are admitted at Ξ±\alpha. Since every pair admitted at Ξ±\alpha is in particular a pair of members of Sym(H)\mathrm{Sym}(H), each instance of the inequality demanded by the second clause is an instance of one supplied by the first, for the same x,y∈Wx,y\in W, the same r∈Rr\in\mathbb{R} with βˆ’R≀r≀R-R\le r\le R and the same Ξ±,δ∈R\alpha,\delta\in\mathbb{R} with 1<Ξ±1<\alpha and 0<Ξ΄<10<\delta<1. Hence (Ο‰1,Ο‰2)(\omega_{1},\omega_{2}) is a second-order structure pair for FF at RR.

Suppose now that FF satisfies the first-order structure condition and let R∈RR\in\mathbb{R} be positive. By The First-Order Structure Condition for a Second-Order Equation Operator on a Hilbert Triple (ii) there is a structure pair for FF at RR, and by the previous paragraph it is a second-order structure pair for FF at RR. 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 (iii).

Proof of claim 2. Let (Nm)m∈N(N_{m})_{m\in\mathbb{N}} be the tail forms of (ek)k∈N(e_{k})_{k\in\mathbb{N}}, which are defined because (ek)k∈N(e_{k})_{k\in\mathbb{N}} is an orthonormal basis of HH all of whose members lie in VV. 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; in particular δ\delta is positive, so A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument (ii) applies to FF with this δ\delta.

For the condition of The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple (iii), let (xm)m∈N(x_{m})_{m\in\mathbb{N}}, (rm)m∈N(r_{m})_{m\in\mathbb{N}}, (pm)m∈N(p_{m})_{m\in\mathbb{N}} and (Xm)m∈N(X_{m})_{m\in\mathbb{N}} be sequences as there. For each m∈Nm\in\mathbb{N} the forms XmX_{m} and Xm+βNmX_{m}+\beta N_{m} both belong to Sym(H)\mathrm{Sym}(H), by Hilbert Triples: Standing Notation and Background (vi), and xm∈Wx_{m}\in W, rm∈Rr_{m}\in\mathbb{R} and pm∈Hp_{m}\in H; so A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument (ii), applied with these data and the two form arguments XmX_{m} and Xm+βNmX_{m}+\beta N_{m}, gives

FΞ΄βˆ’(xm,rm,pm,Xm)=FΞ΄βˆ’(xm,rm,pm,Xm+Ξ²Nm).F^{-}_{\delta}\bigl(x_{m},r_{m},p_{m},X_{m}\bigr)=F^{-}_{\delta}\bigl(x_{m},r_{m},p_{m},X_{m}+\beta N_{m}\bigr).

Since 0<ρ0<\rho, the right-hand side of the inequality required in The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple (iii) exceeds its left-hand side for every m∈Nm\in\mathbb{N}, so that requirement holds with m0=1m_{0}=1.

For the condition of The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple (iv), let the four sequences be as there. The same claim of A First-Order Equation Operator is Degenerate Elliptic and Its Ξ΄\delta-Shifts Ignore the Form Argument, applied with the form arguments Xmβˆ’Ξ²NmX_{m}-\beta N_{m} and XmX_{m}, gives

FΞ΄+(xm,rm,pm,Xmβˆ’Ξ²Nm)=FΞ΄+(xm,rm,pm,Xm),F^{+}_{\delta}\bigl(x_{m},r_{m},p_{m},X_{m}-\beta N_{m}\bigr)=F^{+}_{\delta}\bigl(x_{m},r_{m},p_{m},X_{m}\bigr),

and again 0<ρ0<\rho makes the required inequality hold for every m∈Nm\in\mathbb{N}, so that requirement holds with m0=1m_{0}=1.

As β\beta, RR, ρ\rho and δ\delta were arbitrary subject to the stated restrictions, FF is tail-insensitive along (ek)k∈N(e_{k})_{k\in\mathbb{N}} by The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple (ii).

Proof of claim 3. Since HH is not finite-dimensional, An Orthonormal Basis of the Ambient Space Contained in the Form Space of a Hilbert Triple (i) provides 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}. By claim 2, FF is tail-insensitive along (ek)k∈N(e_{k})_{k\in\mathbb{N}}. Hence FF satisfies the tail-insensitivity condition by The Tail-Insensitivity Condition for an Equation Operator on a Hilbert Triple (v).

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