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The Galerkin Problems of the Wick-Square Problem: Standing Notation for Cubes of Modes, Coordinates, the Free Galerkin Quadratic and the Riccati Potential

Standing notation for the Galerkin problems of the Wick-square problem: for each cutoff an enumeration of the cube of modes, the coordinate map and projection, the free Galerkin quadratic and the Riccati potential.

Statement

This setting fixes the notation of the Galerkin problems of the Wick-square problem. It introduces no new concept and asserts nothing beyond the facts recorded below, each carried by the reference attached to it.

1. (The problem) We work in the settings of The Wick-Square Problem on the Torus: Standing Notation and Second-Order Equations on Euclidean Open Sets. With a mode as subscript, qkq_{k} and aka_{k} are the Riccati coefficients and the renormalised constants, and ckc_{k} are the free-field variances. The Euclidean dimension, written qq in Second-Order Equations on Euclidean Open Sets §space, is written mm below, and the letter qq without a subscript is not used; nor are the letters VV and μ\mu of that setting in their meanings there (an open set, a scalar), VV being reserved for a Sobolev space and μk\mu_{k} for the Fourier weights.

2. (Cutoffs and enumerations) The notation of clauses 2 to 4 is introduced for every N∈NN\in\mathbb{N} simultaneously. The cube ΓN\Gamma_{N} is a nonempty finite set by The Cubes of the Integer Lattice are Finite, Nested, Exhaust the Lattice and Have (2N+1)^n Points §finite, so by Finite Set it has mm elements for a natural number mm, depending on NN, with 1≤m1\le m because ΓN\Gamma_{N} is nonempty; we fix such an mm and a bijection κN\kappa_{N} from the initial segment [m]={1,…,m}[m]=\{1,\dots,m\} onto ΓN\Gamma_{N}.

3. (Coordinates) The coordinate map ιN:Rm→H−1\iota_{N}:\mathbb{R}^{m}\to H^{-1} sends z=(z1,…,zm)z=(z_{1},\dots,z_{m}) to the family with value ziz_{i} at the mode κN(i)\kappa_{N}(i), for each i∈[m]i\in[m], and value 00 at every mode outside ΓN\Gamma_{N}. This family is ∑i=1mzieκN(i)\sum_{i=1}^{m}z_{i}e_{\kappa_{N}(i)}; it lies in H−1H^{-1} because H−1H^{-1} is a linear subspace of Map(Zn,R)\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) (The Wick-Square Problem on the Torus: Standing Notation §state-space) containing the unit families (The Wick-Square Problem on the Torus: Standing Notation §units). The coordinate projection prN:Map(Zn,R)→Rm\mathrm{pr}_{N}:\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R})\to\mathbb{R}^{m} sends xx to (x(κN(1)),…,x(κN(m)))(x(\kappa_{N}(1)),\dots,x(\kappa_{N}(m))), and ΠN=ιN∘prN\Pi_{N}=\iota_{N}\circ\mathrm{pr}_{N} sends xx to the family equal to xx on ΓN\Gamma_{N} and to 00 outside ΓN\Gamma_{N}, which lies in H−1H^{-1}.

4. (The free Galerkin quadratic and the Riccati potential) u~N,ΦN:Rm→R\tilde{u}_{N},\Phi_{N}:\mathbb{R}^{m}\to\mathbb{R} denote the functions

u~N(z)=∑i=1m(qκN(i) zi2+aκN(i)),ΦN(z)=12∑i=1m(μκN(i)+2qκN(i))zi2.\tilde{u}_{N}(z)=\sum_{i=1}^{m}\bigl(q_{\kappa_{N}(i)}\,z_{i}^{2}+a_{\kappa_{N}(i)}\bigr),\qquad\Phi_{N}(z)=\tfrac12\sum_{i=1}^{m}\bigl(\mu_{\kappa_{N}(i)}+2q_{\kappa_{N}(i)}\bigr)z_{i}^{2}.

Both are of class C2C^{2} on Rm\mathbb{R}^{m}, being built from constant and coordinate functions by sums, scalar multiples and products (Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, claims 2 and 3).

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