TheoremBase

Clauses 1, 2 and 5 follow by passing to the limit in the penalised form of the cutoff operators, using the corrector identity LNL_N P = -beta :x2x^2:_N and the convergence results for regular functions. Density comes from replacing the coefficients of y outside a large cube by sqrt(ck)sqrt(c_k). For the absence of interior points, x is perturbed by a small sign-aligned family whose squares have unbounded cube sums: the constant family when n = 1, and muk−1/2mu_k^{-1/2} when n >= 2.

Proof

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

Conventions. Sums over a cube ΓN\Gamma_{N} are sums over a finite index set in the sense of Sum over a Finite Index Set, the cubes being nonempty and finite by The Cubes of the Integer Lattice are Finite, Nested, Exhaust the Lattice and Have (2N+1)^n Points §finite; for a family a:Zn→Ra:\mathbb{Z}^{n}\to\mathbb{R} we write SN(a)=∑k∈ΓNa(k)S_{N}(a)=\sum_{k\in\Gamma_{N}}a(k) for its NNth cube sum, as in Cube Sums of Families on the Integer Lattice §cube-sums. Natural numbers are read in R\mathbb{R} through the canonical map ι\iota, as in The Real Numbers: Standing Notation and Background §numbers. The vector operations of H−1H^{-1} are the pointwise ones, because H−1H^{-1} is a linear subspace of Map(Zn,R)\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) by The Wick-Square Problem on the Torus: Standing Notation §state-space; so for u,v∈H−1u,v\in H^{-1} the vector u−vu-v is the family k↦u(k)−v(k)k\mapsto u(k)-v(k), and by Real Inner Product Space §distance, applied to the inner product of The Negative-Order Sobolev Spaces of the Torus §inner-product, dH−1(u,v)=∣u−v∣H−1d_{H^{-1}}(u,v)=|u-v|_{H^{-1}}, where 0≤∣u−v∣H−10\le|u-v|_{H^{-1}} by Real Inner Product Space §norm. By Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §sobolev with m=1m=1 (as recorded in The Wick-Square Problem on the Torus: Standing Notation §state-space), a family vv lies in H−1H^{-1} exactly when k↦v(k)2/μkk\mapsto v(k)^{2}/\mu_{k} is cube-summable, and then ∣v∣H−12=∑k∈Znv(k)2/μk|v|_{H^{-1}}^{2}=\sum_{k\in\mathbb{Z}^{n}}v(k)^{2}/\mu_{k}.

Preliminary facts.

(C) Constant sequences converge. For a∈Ra\in\mathbb{R}, every ε>0\varepsilon>0 and every N∈NN\in\mathbb{N} we have ∣a−a∣=∣0∣=0<ε|a-a|=|0|=0<\varepsilon by claim 1 of Properties of the Absolute Value in an Ordered Field; so the constant sequence with value aa converges to aa in the sense of Limit of a Sequence of Real Numbers.

(Nn) Products of nonnegative numbers. If 0≤a0\le a and 0≤b0\le b, then a⋅0≤aba\cdot0\le ab by claim 5 of Elementary Arithmetic in an Ordered Field, and a⋅0=0a\cdot0=0 by claim 1 of Zero Products and Elementary Identities in a Field; so 0≤ab0\le ab.

(Sq) Squares are nonnegative. Let r∈Rr\in\mathbb{R}. If 0≤r0\le r, then 0≤r20\le r^{2} by (Nn). Otherwise r≤0r\le0, the order being total, so 0≤−r0\le-r by claim 4 of Elementary Order Arithmetic in an Ordered Field, and r2=(−r)(−r)r^{2}=(-r)(-r) by claim 2 of Zero Products and Elementary Identities in a Field, which is nonnegative by (Nn).

(Tw) A bound for the square of a difference. Let p,q∈Rp,q\in\mathbb{R}. By claim 5 of Zero Products and Elementary Identities in a Field, (p+q)2=p2+(pq+pq)+q2(p+q)^{2}=p^{2}+(pq+pq)+q^{2}, and, applied to pp and −q-q together with claim 2 of that lemma, (p−q)2=p2−(pq+pq)+q2(p-q)^{2}=p^{2}-(pq+pq)+q^{2}. Adding, (p−q)2+(p+q)2=2(p2+q2)(p-q)^{2}+(p+q)^{2}=2(p^{2}+q^{2}), so 2(p2+q2)−(p−q)2=(p+q)22(p^{2}+q^{2})-(p-q)^{2}=(p+q)^{2}, which is nonnegative by (Sq); hence (p−q)2≤2(p2+q2)(p-q)^{2}\le2(p^{2}+q^{2}) by claim 3 of Elementary Arithmetic in an Ordered Field.

(Wt) The weights and the variances. For every mode kk: 1≤μk1\le\mu_{k} by The Wick-Square Problem on the Torus: Standing Notation §modes and 0<10<1 by claim 6 of Elementary Order Arithmetic in an Ordered Field, so 0<μk0<\mu_{k} by claim 2 of that lemma and 0<μk−10<\mu_{k}^{-1} by its claim 7. Also 0<ck0<c_{k} and ck=ν(2μk)−1c_{k}=\nu(2\mu_{k})^{-1} by The Free-Field Variances of the Fourier Modes §variances. Since in a field the inverse of a product of nonzero elements is the product of the inverses, and μk2=μkμk\mu_{k}^{2}=\mu_{k}\mu_{k} (The Real Numbers: Standing Notation and Background §numbers),

ck=ν2 μk−1,ckμk=ν2⋅1μk2.c_{k}=\frac{\nu}{2}\,\mu_{k}^{-1},\qquad \frac{c_{k}}{\mu_{k}}=\frac{\nu}{2}\cdot\frac{1}{\mu_{k}^{2}}.

Since n≤3<4n\le3<4 by The Wick-Square Problem on the Torus: Standing Notation §dimension, the family k↦1/μk2k\mapsto1/\mu_{k}^{2} is cube-summable by Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §convergent with s=2s=2, and therefore so is k↦ck/μkk\mapsto c_{k}/\mu_{k}, by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §linear with λ=ν/2\lambda=\nu/2.

Clause 1 (penalised). Let ψ=φ−P\psi=\varphi-P, the function u↦φ(u)−P(u)u\mapsto\varphi(u)-P(u) on H−1H^{-1}; it is regular by hypothesis, so by Regular Functions for the Wick-Square Problem: Diagonal Quadratics of Curvature of Order the Inverse Squared Weight, plus Twice Differentiable Functions on the Sobolev Space of Order -3 it has a curvature family and a cylindrical part, which we fix, and Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations applies to ψ\psi. For every u∈H−1u\in H^{-1} we have 1⋅P(u)+ψ(u)=φ(u)1\cdot P(u)+\psi(u)=\varphi(u), so φ=θP+ψ\varphi=\theta P+\psi with θ=1\theta=1. By Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations §gradient with θ=1\theta=1, φ\varphi is twice differentiable along the modes and ∣Dφ(x)∣2|D\varphi(x)|^{2} is defined for every x∈H−1x\in H^{-1}; that is, by The Gradient Energy with a Mode Cutoff §limit, the sequence (∣DNφ(x)∣2)N∈N(|D_{N}\varphi(x)|^{2})_{N\in\mathbb{N}} converges to ∣Dφ(x)∣2|D\varphi(x)|^{2}.

Fix x∈H−1x\in H^{-1}. By Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations §generator, Lψ=L(φ−P)L\psi=L(\varphi-P) is defined at xx, that is, by The Free-Field Generator with a Mode Cutoff §limit, the sequence (LN(φ−P)(x))N∈N(L_{N}(\varphi-P)(x))_{N\in\mathbb{N}} converges to L(φ−P)(x)L(\varphi-P)(x). Since φ\varphi is twice differentiable along the modes, The Cutoff Wick Square is Minus the Free-Field Generator of the Gaussian Penalty, and the Penalised Form of the Cutoff Operators §penalised gives, for every N∈NN\in\mathbb{N},

FN[φ](x)=γ φ(x)−LN(φ−P)(x)+12 ∣DNφ(x)∣2−g(x).F_{N}[\varphi](x)=\gamma\,\varphi(x)-L_{N}(\varphi-P)(x)+\tfrac12\,|D_{N}\varphi(x)|^{2}-g(x).

The constant sequences with values γφ(x)\gamma\varphi(x) and g(x)g(x) converge by (C). By claims 1 and 3 of Arithmetic of Limits of Real Sequences, the right-hand side converges, as N→∞N\to\infty, to γφ(x)−L(φ−P)(x)+12∣Dφ(x)∣2−g(x)\gamma\varphi(x)-L(\varphi-P)(x)+\tfrac12|D\varphi(x)|^{2}-g(x). Hence (FN[φ](x))N∈N(F_{N}[\varphi](x))_{N\in\mathbb{N}} converges, so (φ,x)∈D(\varphi,x)\in\mathcal{D} by The Renormalised Hamilton-Jacobi-Bellman Operator of the Wick-Square Problem as the Limit of the Wick-Ordered Cutoff Operators §domain, and by The Renormalised Hamilton-Jacobi-Bellman Operator of the Wick-Square Problem as the Limit of the Wick-Ordered Cutoff Operators §operator together with claim 1 of Uniqueness of Limits and Boundedness of Convergent Real Sequences, F[φ](x)F[\varphi](x) equals this limit, which is the asserted formula.

Clause 2 (wick-only). Let ψ=φ−θP\psi=\varphi-\theta P, regular by hypothesis; fix a curvature family and a cylindrical part of it as in Clause 1. For every u∈H−1u\in H^{-1}, φ(u)=θP(u)+ψ(u)\varphi(u)=\theta P(u)+\psi(u), so Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations §gradient, applied with this θ\theta, shows that φ\varphi is twice differentiable along the modes and that (∣DNφ(x)∣2)N∈N(|D_{N}\varphi(x)|^{2})_{N\in\mathbb{N}} converges for every x∈H−1x\in H^{-1} (The Gradient Energy with a Mode Cutoff §limit).

Let h=φ−Ph=\varphi-P. For every u∈H−1u\in H^{-1}, h(u)=(θ−1)P(u)+ψ(u)h(u)=(\theta-1)P(u)+\psi(u). Mode derivatives of hh. Fix x∈H−1x\in H^{-1} and a mode kk, and let σh,σP,σψ:R→R\sigma^{h},\sigma^{P},\sigma^{\psi}:\mathbb{R}\to\mathbb{R} be the sections of hh, PP and ψ\psi at xx along kk (Derivatives of a Function on the Sobolev Space of Order -1 along the Fourier Modes); then σh(s)=(θ−1)σP(s)+σψ(s)\sigma^{h}(s)=(\theta-1)\sigma^{P}(s)+\sigma^{\psi}(s) for every s∈Rs\in\mathbb{R}. The function PP is twice differentiable along the modes by The Cutoff Wick Square is Minus the Free-Field Generator of the Gaussian Penalty, and the Penalised Form of the Cutoff Operators §derivatives, and ψ\psi by Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations §derivatives; so, by Derivatives of a Function on the Sobolev Space of Order -1 along the Fourier Modes §twice, σP\sigma^{P} and σψ\sigma^{\psi} are differentiable at every point of R\mathbb{R} and their derivatives are differentiable at 00. By claim 2 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives, applied on the interval R\mathbb{R}, all of whose points are interior points, first to (θ−1)σP(\theta-1)\sigma^{P} and then to the sum, σh\sigma^{h} is differentiable at every s∈Rs\in\mathbb{R} with (σh)′(s)=(θ−1)(σP)′(s)+(σψ)′(s)(\sigma^{h})'(s)=(\theta-1)(\sigma^{P})'(s)+(\sigma^{\psi})'(s); thus (σh)′=(θ−1)(σP)′+(σψ)′(\sigma^{h})'=(\theta-1)(\sigma^{P})'+(\sigma^{\psi})' as functions on R\mathbb{R}, and the same claim applied at 00 gives ((σh)′)′(0)=(θ−1)((σP)′)′(0)+((σψ)′)′(0)((\sigma^{h})')'(0)=(\theta-1)((\sigma^{P})')'(0)+((\sigma^{\psi})')'(0). By Derivatives of a Function on the Sobolev Space of Order -1 along the Fourier Modes §derivatives,

∂kh(x)=(θ−1) ∂kP(x)+∂kψ(x),∂k2h(x)=(θ−1) ∂k2P(x)+∂k2ψ(x).\partial_{k}h(x)=(\theta-1)\,\partial_{k}P(x)+\partial_{k}\psi(x),\qquad\partial_{k}^{2}h(x)=(\theta-1)\,\partial_{k}^{2}P(x)+\partial_{k}^{2}\psi(x).

The generator of hh. Fix x∈H−1x\in H^{-1} and N∈NN\in\mathbb{N}. By the displayed identities and the field axioms, for every k∈ΓNk\in\Gamma_{N} the summand ν2∂k2h(x)−μkx(k)∂kh(x)\tfrac{\nu}{2}\partial_{k}^{2}h(x)-\mu_{k}x(k)\partial_{k}h(x) of LNh(x)L_{N}h(x) (The Free-Field Generator with a Mode Cutoff §generator) equals (θ−1)(ν2∂k2P(x)−μkx(k)∂kP(x))+(ν2∂k2ψ(x)−μkx(k)∂kψ(x))(\theta-1)\bigl(\tfrac{\nu}{2}\partial_{k}^{2}P(x)-\mu_{k}x(k)\partial_{k}P(x)\bigr)+\bigl(\tfrac{\nu}{2}\partial_{k}^{2}\psi(x)-\mu_{k}x(k)\partial_{k}\psi(x)\bigr). Summing over ΓN\Gamma_{N} with claims 3 and 4 of Properties of a Sum over a Finite Index Set, and then using The Cutoff Wick Square is Minus the Free-Field Generator of the Gaussian Penalty, and the Penalised Form of the Cutoff Operators §corrector,

LN(φ−P)(x)=(θ−1) LNP(x)+LNψ(x)=−(θ−1)β :x2:N+LNψ(x).L_{N}(\varphi-P)(x)=(\theta-1)\,L_{N}P(x)+L_{N}\psi(x)=-(\theta-1)\beta\,{:}x^{2}{:}_{N}+L_{N}\psi(x).

The cutoff operators. Put λ=(θ−1)β\lambda=(\theta-1)\beta and AN=γφ(x)−LNψ(x)+12∣DNφ(x)∣2−g(x)A_{N}=\gamma\varphi(x)-L_{N}\psi(x)+\tfrac12|D_{N}\varphi(x)|^{2}-g(x). By The Cutoff Wick Square is Minus the Free-Field Generator of the Gaussian Penalty, and the Penalised Form of the Cutoff Operators §penalised (applicable since φ\varphi is twice differentiable along the modes) and the last display, for every N∈NN\in\mathbb{N}

FN[φ](x)=AN+λ :x2:N.F_{N}[\varphi](x)=A_{N}+\lambda\,{:}x^{2}{:}_{N}.

The sequence (AN)N∈N(A_{N})_{N\in\mathbb{N}} converges: (LNψ(x))N(L_{N}\psi(x))_{N} converges by Regular Functions: Mode Derivatives, the Free-Field Generator, the Gradient Energy, the Renormalised Operator at the Gaussian Penalty plus a Regular Function, and Linear Combinations §generator and The Free-Field Generator with a Mode Cutoff §limit, (∣DNφ(x)∣2)N(|D_{N}\varphi(x)|^{2})_{N} converges as shown above, the constant sequences converge by (C), and claims 1 and 3 of Arithmetic of Limits of Real Sequences apply. Moreover λ≠0\lambda\ne0: θ−1≠0\theta-1\ne0 because θ≠1\theta\ne1, β≠0\beta\ne0 because 0<β0<\beta (The Wick-Square Problem on the Torus: Standing Notation §parameters), and claim 3 of Zero Products and Elementary Identities in a Field applies.

If x∈Wx\in\mathcal{W}, then (:x2:N)N({:}x^{2}{:}_{N})_{N} converges by The Wick Square with a Mode Cutoff and the Wick Domain §domain, so (FN[φ](x))N(F_{N}[\varphi](x))_{N} converges by claims 1 and 3 of Arithmetic of Limits of Real Sequences, and (φ,x)∈D(\varphi,x)\in\mathcal{D} by The Renormalised Hamilton-Jacobi-Bellman Operator of the Wick-Square Problem as the Limit of the Wick-Ordered Cutoff Operators §domain. Conversely, if (φ,x)∈D(\varphi,x)\in\mathcal{D}, then (FN[φ](x))N(F_{N}[\varphi](x))_{N} converges, and :x2:N=λ−1(FN[φ](x)−AN){:}x^{2}{:}_{N}=\lambda^{-1}\bigl(F_{N}[\varphi](x)-A_{N}\bigr) for every NN, so (:x2:N)N({:}x^{2}{:}_{N})_{N} converges by claim 3 of Arithmetic of Limits of Real Sequences; as x∈H−1x\in H^{-1}, this gives x∈Wx\in\mathcal{W} by The Wick Square with a Mode Cutoff and the Wick Domain §domain.

Clause 3 (dense). Let y∈H−1y\in H^{-1} and ε>0\varepsilon>0 be given. The order of choice is: first η\eta (depending on ε\varepsilon), then MM (depending on yy and η\eta), then zz (depending on yy and MM).

The tail family. Let a(k)=y(k)2/μka(k)=y(k)^{2}/\mu_{k} and h(k)=a(k)+ck/μkh(k)=a(k)+c_{k}/\mu_{k} for k∈Znk\in\mathbb{Z}^{n}. The family aa is cube-summable since y∈H−1y\in H^{-1} (Conventions), and k↦ck/μkk\mapsto c_{k}/\mu_{k} is cube-summable by (Wt); so hh is cube-summable by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §linear, with lattice sum S=∑k∈Znh(k)S=\sum_{k\in\mathbb{Z}^{n}}h(k). Also 0≤h(k)0\le h(k) for every kk, by (Sq), (Wt), (Nn) and claim 2 of Elementary Arithmetic in an Ordered Field.

Choice of η\eta and MM. Since 0<ε0<\varepsilon, 0<ε20<\varepsilon^{2} by claim 5 of Elementary Order Arithmetic in an Ordered Field; put ε′=ε2⋅2−1\varepsilon'=\varepsilon^{2}\cdot2^{-1} and η=ε′⋅2−1\eta=\varepsilon'\cdot2^{-1}, so that by claim 8 of that lemma (twice) 0<η0<\eta, η+η=ε′\eta+\eta=\varepsilon' and ε′<ε2\varepsilon'<\varepsilon^{2}. Since (SN(h))N(S_{N}(h))_{N} converges to SS (Cube Sums of Families on the Integer Lattice §lattice-sum), Limit of a Sequence of Real Numbers applied with η\eta provides M∈NM\in\mathbb{N} with ∣SN(h)−S∣<η|S_{N}(h)-S|<\eta for all N≥MN\ge M; in particular ∣SM(h)−S∣<η|S_{M}(h)-S|<\eta.

Definition of zz. For k∉ΓMk\notin\Gamma_{M} let rkr_{k} be the real number with 0≤rk0\le r_{k} and rk2=ckr_{k}^{2}=c_{k} given by Existence and Uniqueness of the Nonnegative Square Root (applicable since 0<ck0<c_{k} by (Wt)). Let z(k)=y(k)z(k)=y(k) for k∈ΓMk\in\Gamma_{M} and z(k)=rkz(k)=r_{k} for k∉ΓMk\notin\Gamma_{M}, and let vv be the family k↦y(k)−z(k)k\mapsto y(k)-z(k); so v(k)=0v(k)=0 for k∈ΓMk\in\Gamma_{M} and v(k)=y(k)−rkv(k)=y(k)-r_{k} otherwise.

A dominating family. Let hM(k)=h(k)h_{M}(k)=h(k) for k∈ΓMk\in\Gamma_{M} and hM(k)=0h_{M}(k)=0 otherwise. Since ΓM\Gamma_{M} is nonempty and finite, Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §finite-support shows that hMh_{M} is cube-summable with lattice sum ∑k∈ΓMhM(k)=∑k∈ΓMh(k)=SM(h)\sum_{k\in\Gamma_{M}}h_{M}(k)=\sum_{k\in\Gamma_{M}}h(k)=S_{M}(h) (the two maps agree on ΓM\Gamma_{M}). Let e=2h−2hMe=2h-2h_{M}; by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §linear it is cube-summable with ∑k∈Zne(k)=2(S−SM(h))\sum_{k\in\mathbb{Z}^{n}}e(k)=2(S-S_{M}(h)), and e(k)=0e(k)=0 for k∈ΓMk\in\Gamma_{M}, e(k)=2h(k)e(k)=2h(k) otherwise. We claim 0≤v(k)2/μk≤e(k)0\le v(k)^{2}/\mu_{k}\le e(k) for every kk. Nonnegativity follows from (Sq), (Wt) and (Nn). For k∈ΓMk\in\Gamma_{M}, v(k)2/μk=0=e(k)v(k)^{2}/\mu_{k}=0=e(k). For k∉ΓMk\notin\Gamma_{M}, (Tw) with p=y(k)p=y(k), q=rkq=r_{k} gives v(k)2≤2(y(k)2+rk2)=2(y(k)2+ck)v(k)^{2}\le2(y(k)^{2}+r_{k}^{2})=2(y(k)^{2}+c_{k}), and multiplying by μk−1\mu_{k}^{-1}, which is nonnegative by (Wt), claim 5 of Elementary Arithmetic in an Ordered Field gives v(k)2/μk≤2(a(k)+ck/μk)=e(k)v(k)^{2}/\mu_{k}\le2(a(k)+c_{k}/\mu_{k})=e(k). Since ∣v(k)2/μk∣=v(k)2/μk|v(k)^{2}/\mu_{k}|=v(k)^{2}/\mu_{k} by Absolute Value in an Ordered Field, Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §comparison shows that k↦v(k)2/μkk\mapsto v(k)^{2}/\mu_{k} is cube-summable with ∑k∈Znv(k)2/μk≤2(S−SM(h))\sum_{k\in\mathbb{Z}^{n}}v(k)^{2}/\mu_{k}\le2(S-S_{M}(h)).

z∈H−1z\in H^{-1} and the distance. By the Conventions, v∈H−1v\in H^{-1} and ∣v∣H−12≤2(S−SM(h))|v|_{H^{-1}}^{2}\le2(S-S_{M}(h)). As z(k)=y(k)−v(k)z(k)=y(k)-v(k) for every kk and H−1H^{-1} is a linear subspace, z=y−v∈H−1z=y-v\in H^{-1}, and y−z=vy-z=v, so dH−1(y,z)=∣v∣H−1d_{H^{-1}}(y,z)=|v|_{H^{-1}}. Now S−SM(h)=−(SM(h)−S)≤∣SM(h)−S∣S-S_{M}(h)=-(S_{M}(h)-S)\le|S_{M}(h)-S| by claims 2 and 3 of Properties of the Absolute Value in an Ordered Field; multiplying by 2≥02\ge0 (claim 5 of Elementary Arithmetic in an Ordered Field), and then using ∣SM(h)−S∣<η|S_{M}(h)-S|<\eta with 0<20<2 and claim 10 of Elementary Order Arithmetic in an Ordered Field, we get ∣v∣H−12≤2(S−SM(h))≤2∣SM(h)−S∣<2η=η+η=ε′<ε2|v|_{H^{-1}}^{2}\le2(S-S_{M}(h))\le2|S_{M}(h)-S|<2\eta=\eta+\eta=\varepsilon'<\varepsilon^{2}, the strict links combining by claim 2 of that lemma. Since 0≤∣v∣H−10\le|v|_{H^{-1}} and 0≤ε0\le\varepsilon, claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives dH−1(y,z)=∣v∣H−1<εd_{H^{-1}}(y,z)=|v|_{H^{-1}}<\varepsilon.

z∈Wz\in\mathcal{W}. Let q(k)=z(k)2−ckq(k)=z(k)^{2}-c_{k}. For k∉ΓMk\notin\Gamma_{M}, q(k)=rk2−ck=0q(k)=r_{k}^{2}-c_{k}=0. By Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §finite-support with E=ΓME=\Gamma_{M}, the family qq is cube-summable, i.e. (SN(q))N(S_{N}(q))_{N} converges. By The Wick Square with a Mode Cutoff and the Wick Domain §cutoff, SN(q)=:z2:NS_{N}(q)={:}z^{2}{:}_{N} for every NN, so (:z2:N)N({:}z^{2}{:}_{N})_{N} converges and, as z∈H−1z\in H^{-1}, z∈Wz\in\mathcal{W} by The Wick Square with a Mode Cutoff and the Wick Domain §domain.

Clause 4 (no-interior). Let x∈H−1x\in H^{-1} and ε>0\varepsilon>0 be given. If x∉Wx\notin\mathcal{W}, take z=xz=x: then dH−1(x,x)=0<εd_{H^{-1}}(x,x)=0<\varepsilon, because dH−1d_{H^{-1}} is a metric (The Negative-Order Sobolev Spaces of the Torus §inner-product, The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §metric) and condition 2 of Metric Space holds. Assume from now on that x∈Wx\in\mathcal{W}. The order of choice is: the weight family ww (depending only on nn) and the signs sks_{k} (depending on xx); then the number AA; then ρ\rho and tt (depending on AA and ε\varepsilon); then zz.

The weight family. If n=1n=1, let w(k)=1w(k)=1 for every kk. If 2≤n2\le n, let w(k)w(k) be the real number with 0≤w(k)0\le w(k) and w(k)2=μk−1w(k)^{2}=\mu_{k}^{-1}, given by Existence and Uniqueness of the Nonnegative Square Root since 0<μk−10<\mu_{k}^{-1} by (Wt). In either case 0≤w(k)0\le w(k) for every kk (claim 1 of Elementary Arithmetic in an Ordered Field when n=1n=1), and ww has the following two properties.

(W2) The family k↦w(k)2/μkk\mapsto w(k)^{2}/\mu_{k} is cube-summable. If n=1n=1, it is k↦1/μk=1/μk1k\mapsto1/\mu_{k}=1/\mu_{k}^{1}, cube-summable by Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §convergent with s=1s=1, since 1<21<2. If 2≤n2\le n, it is k↦μk−1μk−1=1/μk2k\mapsto\mu_{k}^{-1}\mu_{k}^{-1}=1/\mu_{k}^{2}, cube-summable by (Wt).

(W3) The set {SN(w2):N∈N}\{S_{N}(w^{2}):N\in\mathbb{N}\}, where w2w^{2} is the family k↦w(k)2k\mapsto w(k)^{2}, is not bounded above. If 2≤n2\le n, SN(w2)=∑k∈ΓN1/μkS_{N}(w^{2})=\sum_{k\in\Gamma_{N}}1/\mu_{k} and this is Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §divergent. Let n=1n=1; then w(k)2=1w(k)^{2}=1 for all kk, and a mode is a map on [1][1], determined by its single component. For N∈NN\in\mathbb{N} let qNq_{N} be the mode with component NN. Since −N≤N≤N-N\le N\le N in the integers, qN∈ΓNq_{N}\in\Gamma_{N}; since N<N+1N<N+1, qN+1∉ΓNq_{N+1}\notin\Gamma_{N}. Let TT be the set of N∈NN\in\mathbb{N} with ι(N)≤SN(w2)\iota(N)\le S_{N}(w^{2}). The constant family 11 is nonnegative (claim 1 of Elementary Arithmetic in an Ordered Field). By the monotonicity claim Real Sums over a Finite Index Set: Comparison, Nonnegativity, Monotonicity, Term Bounds, Absolute Values, Counting and Limits §monotone with E={q1}⊆Γ1E=\{q_{1}\}\subseteq\Gamma_{1}, claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set and claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field, ι(1)=1=∑k∈{q1}1≤S1(w2)\iota(1)=1=\sum_{k\in\{q_{1}\}}1\le S_{1}(w^{2}), so 1∈T1\in T. Let N∈TN\in T. As N≤N+1N\le N+1, ΓN⊆ΓN+1\Gamma_{N}\subseteq\Gamma_{N+1} by The Cubes of the Integer Lattice are Finite, Nested, Exhaust the Lattice and Have (2N+1)^n Points §nested, and qN+1∈ΓN+1∖ΓNq_{N+1}\in\Gamma_{N+1}\setminus\Gamma_{N}; so by Real Sums over a Finite Index Set: Comparison, Nonnegativity, Monotonicity, Term Bounds, Absolute Values, Counting and Limits §monotone with E=ΓN∪{qN+1}E=\Gamma_{N}\cup\{q_{N+1}\}, and by claim 2 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, SN+1(w2)≥∑k∈ΓN∪{qN+1}1=SN(w2)+1≥ι(N)+1=ι(N+1)S_{N+1}(w^{2})\ge\sum_{k\in\Gamma_{N}\cup\{q_{N+1}\}}1=S_{N}(w^{2})+1\ge\iota(N)+1=\iota(N+1), using N∈TN\in T and claim 3 of Elementary Arithmetic in an Ordered Field for the second inequality and claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field for the equality. Thus N+1∈TN+1\in T, and T=NT=\mathbb{N} by Principle of Induction for the Natural Numbers (with S(N)=N+1S(N)=N+1, Natural Numbers). If some real BB satisfied SN(w2)≤BS_{N}(w^{2})\le B for all NN, claim 1 of The Archimedean Property of the Real Numbers would give NN with B<ι(N)B<\iota(N), and then ι(N)≤SN(w2)≤B<ι(N)\iota(N)\le S_{N}(w^{2})\le B<\iota(N), so ι(N)<ι(N)\iota(N)<\iota(N) by claim 2 of Elementary Order Arithmetic in an Ordered Field, which is absurd.

Signs, AA and tt. For each kk let sk=1s_{k}=1 if 0≤x(k)0\le x(k) and sk=−1s_{k}=-1 otherwise. Then 0≤skx(k)0\le s_{k}x(k) (in the second case x(k)≤0x(k)\le0 and claim 4 of Elementary Order Arithmetic in an Ordered Field applies), and sk2=1s_{k}^{2}=1 by claim 2 of Zero Products and Elementary Identities in a Field. Let A=∑k∈Znw(k)2/μkA=\sum_{k\in\mathbb{Z}^{n}}w(k)^{2}/\mu_{k}, which exists by (W2) and satisfies 0≤A0\le A by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §nonnegative, the family being nonnegative by (Sq), (Wt) and (Nn). Then 0<A+10<A+1 by claim 3 of Elementary Order Arithmetic in an Ordered Field (from 0<10<1 and 0≤A0\le A), so 0<(A+1)−10<(A+1)^{-1} by claim 7 of that lemma; let ρ\rho be the real number with 0≤ρ0\le\rho and ρ2=(A+1)−1\rho^{2}=(A+1)^{-1} (Existence and Uniqueness of the Nonnegative Square Root). Then ρ≠0\rho\ne0, since otherwise ρ2=0\rho^{2}=0 by claim 1 of Zero Products and Elementary Identities in a Field; so 0<ρ0<\rho, and t=ερt=\varepsilon\rho satisfies 0<t0<t by claim 5 of Elementary Order Arithmetic in an Ordered Field, and t2=ε2(A+1)−1t^{2}=\varepsilon^{2}(A+1)^{-1}.

Definition of zz and the distance. Let u(k)=skw(k)u(k)=s_{k}w(k) and let δ\delta be the family k↦t u(k)k\mapsto t\,u(k). For every kk, δ(k)2/μk=t2sk2w(k)2/μk=t2 w(k)2/μk\delta(k)^{2}/\mu_{k}=t^{2}s_{k}^{2}w(k)^{2}/\mu_{k}=t^{2}\,w(k)^{2}/\mu_{k}, so by (W2) and Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §linear the family k↦δ(k)2/μkk\mapsto\delta(k)^{2}/\mu_{k} is cube-summable with lattice sum t2At^{2}A; by the Conventions δ∈H−1\delta\in H^{-1}, and z=x+δ∈H−1z=x+\delta\in H^{-1} as H−1H^{-1} is a linear subspace. The vector x−zx-z is the family k↦−δ(k)k\mapsto-\delta(k), and (−δ(k))2=δ(k)2(-\delta(k))^{2}=\delta(k)^{2} by claim 2 of Zero Products and Elementary Identities in a Field; so by the Conventions dH−1(x,z)2=∣x−z∣H−12=t2A=ε2⋅A(A+1)−1d_{H^{-1}}(x,z)^{2}=|x-z|_{H^{-1}}^{2}=t^{2}A=\varepsilon^{2}\cdot A(A+1)^{-1}. From A<A+1A<A+1 (claim 1 of Elementary Order Arithmetic in an Ordered Field, from 0<10<1) and 0<(A+1)−10<(A+1)^{-1}, claim 10 of that lemma gives A(A+1)−1<(A+1)(A+1)−1=1A(A+1)^{-1}<(A+1)(A+1)^{-1}=1, and again, with 0<ε20<\varepsilon^{2} (claim 5), ε2A(A+1)−1<ε2\varepsilon^{2}A(A+1)^{-1}<\varepsilon^{2}. As 0≤dH−1(x,z)0\le d_{H^{-1}}(x,z) and 0≤ε0\le\varepsilon, claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field yields dH−1(x,z)<εd_{H^{-1}}(x,z)<\varepsilon.

z∉Wz\notin\mathcal{W}. Fix kk. By claim 5 of Zero Products and Elementary Identities in a Field, z(k)2=x(k)2+(x(k)δ(k)+x(k)δ(k))+δ(k)2z(k)^{2}=x(k)^{2}+\bigl(x(k)\delta(k)+x(k)\delta(k)\bigr)+\delta(k)^{2}. Here x(k)δ(k)=t w(k) (skx(k))x(k)\delta(k)=t\,w(k)\,\bigl(s_{k}x(k)\bigr) is nonnegative by (Nn) applied twice (with 0≤t0\le t, 0≤w(k)0\le w(k), 0≤skx(k)0\le s_{k}x(k)), so 0≤x(k)δ(k)+x(k)δ(k)0\le x(k)\delta(k)+x(k)\delta(k) by claim 2 of Elementary Arithmetic in an Ordered Field; and δ(k)2=t2w(k)2\delta(k)^{2}=t^{2}w(k)^{2}. Hence, by claim 3 of that lemma, (x(k)2−ck)+t2w(k)2≤z(k)2−ck\bigl(x(k)^{2}-c_{k}\bigr)+t^{2}w(k)^{2}\le z(k)^{2}-c_{k}. Summing over ΓN\Gamma_{N} with Real Sums over a Finite Index Set: Comparison, Nonnegativity, Monotonicity, Term Bounds, Absolute Values, Counting and Limits §comparison and claims 3 and 4 of Properties of a Sum over a Finite Index Set, and using The Wick Square with a Mode Cutoff and the Wick Domain §cutoff,

:x2:N+t2SN(w2)≤:z2:N(N∈N).{:}x^{2}{:}_{N}+t^{2}S_{N}(w^{2})\le{:}z^{2}{:}_{N}\qquad(N\in\mathbb{N}).

Suppose z∈Wz\in\mathcal{W}. Then (:x2:N)N({:}x^{2}{:}_{N})_{N} and (:z2:N)N({:}z^{2}{:}_{N})_{N} both converge (The Wick Square with a Mode Cutoff and the Wick Domain §domain), hence are bounded by claim 2 of Uniqueness of Limits and Boundedness of Convergent Real Sequences: by Bounded Sequence of Real Numbers there are reals R1,R2>0R_{1},R_{2}>0 with ∣:x2:N∣≤R1|{:}x^{2}{:}_{N}|\le R_{1} and ∣:z2:N∣≤R2|{:}z^{2}{:}_{N}|\le R_{2} for all NN. By claims 2 and 3 of Properties of the Absolute Value in an Ordered Field and claim 4 of Elementary Order Arithmetic in an Ordered Field, :z2:N≤R2{:}z^{2}{:}_{N}\le R_{2} and −:x2:N≤R1-{:}x^{2}{:}_{N}\le R_{1}, so, adding (claims 2 and 3 of Elementary Arithmetic in an Ordered Field), t2SN(w2)≤:z2:N−:x2:N≤R1+R2t^{2}S_{N}(w^{2})\le{:}z^{2}{:}_{N}-{:}x^{2}{:}_{N}\le R_{1}+R_{2}. Since 0<t20<t^{2} (claim 5 of Elementary Order Arithmetic in an Ordered Field), 0<(t2)−10<(t^{2})^{-1} by claim 7 of that lemma, and claim 5 of Elementary Arithmetic in an Ordered Field gives SN(w2)≤(t2)−1(R1+R2)S_{N}(w^{2})\le(t^{2})^{-1}(R_{1}+R_{2}) for every NN, so {SN(w2):N∈N}\{S_{N}(w^{2}):N\in\mathbb{N}\} is bounded above (Upper Bound and Least Upper Bound), contradicting (W3). Hence z∉Wz\notin\mathcal{W}, and zz has the required properties.

Clause 5 (counterterm). Let bb, φ\varphi and xx be as stated. By Clause 1, φ\varphi is twice differentiable along the modes and (FN[φ](x))N(F_{N}[\varphi](x))_{N} converges. Subtracting the two identities of The Cutoff Wick Square is Minus the Free-Field Generator of the Gaussian Penalty, and the Penalised Form of the Cutoff Operators §penalised, for every N∈NN\in\mathbb{N}

FNb[φ](x)=FN[φ](x)−β SN(c−b),F_{N}^{b}[\varphi](x)=F_{N}[\varphi](x)-\beta\,S_{N}(c-b),

where c−bc-b is the family k↦ck−b(k)k\mapsto c_{k}-b(k). If c−bc-b is cube-summable, i.e. (SN(c−b))N(S_{N}(c-b))_{N} converges (Cube Sums of Families on the Integer Lattice §lattice-sum), then (FNb[φ](x))N(F_{N}^{b}[\varphi](x))_{N} converges by claims 1 and 3 of Arithmetic of Limits of Real Sequences. Conversely, if (FNb[φ](x))N(F_{N}^{b}[\varphi](x))_{N} converges, then, as β≠0\beta\ne0 (since 0<β0<\beta, The Wick-Square Problem on the Torus: Standing Notation §parameters), SN(c−b)=β−1(FN[φ](x)−FNb[φ](x))S_{N}(c-b)=\beta^{-1}\bigl(F_{N}[\varphi](x)-F_{N}^{b}[\varphi](x)\bigr) converges by claim 3 of Arithmetic of Limits of Real Sequences, so c−bc-b is cube-summable.

Now let 2≤n2\le n and bb be the zero family, so that FNb=FN0F_{N}^{b}=F_{N}^{0} (The Cutoff Hamilton-Jacobi-Bellman Operators of the Wick-Square Problem, with a General Counterterm §bare) and c−b=cc-b=c. By (Wt) and claim 4 of Properties of a Sum over a Finite Index Set, βSN(c)=κ TN\beta S_{N}(c)=\kappa\,T_{N} with κ=βν 2−1\kappa=\beta\nu\,2^{-1} and TN=∑k∈ΓN1/μkT_{N}=\sum_{k\in\Gamma_{N}}1/\mu_{k}; here 0<κ0<\kappa by claims 8 and 5 of Elementary Order Arithmetic in an Ordered Field, since 0<β0<\beta and 0<ν0<\nu. Suppose (FN0[φ](x))N(F_{N}^{0}[\varphi](x))_{N} were bounded below, i.e. (The Real Numbers: Standing Notation and Background §bounds, Lower Bound and Greatest Lower Bound in a Totally Ordered Set) there were a real ℓ\ell with ℓ≤FN0[φ](x)\ell\le F_{N}^{0}[\varphi](x) for all NN. Since (FN[φ](x))N(F_{N}[\varphi](x))_{N} converges, it is bounded (claim 2 of Uniqueness of Limits and Boundedness of Convergent Real Sequences): there is R>0R>0 with ∣FN[φ](x)∣≤R|F_{N}[\varphi](x)|\le R, hence FN[φ](x)≤RF_{N}[\varphi](x)\le R by claim 3 of Properties of the Absolute Value in an Ordered Field, for all NN. With −FN0[φ](x)≤−ℓ-F_{N}^{0}[\varphi](x)\le-\ell (claim 4 of Elementary Order Arithmetic in an Ordered Field) and claims 2 and 3 of Elementary Arithmetic in an Ordered Field, κTN=FN[φ](x)−FN0[φ](x)≤R−ℓ\kappa T_{N}=F_{N}[\varphi](x)-F_{N}^{0}[\varphi](x)\le R-\ell, and, multiplying by κ−1\kappa^{-1}, which is positive by claim 7 of Elementary Order Arithmetic in an Ordered Field, claim 5 of Elementary Arithmetic in an Ordered Field gives TN≤κ−1(R−ℓ)T_{N}\le\kappa^{-1}(R-\ell) for every NN. So {TN:N∈N}\{T_{N}:N\in\mathbb{N}\} would be bounded above, contradicting Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §divergent. Hence (FN0[φ](x))N(F_{N}^{0}[\varphi](x))_{N} is not bounded below.

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