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The Wick-Ordered Phi4Phi^4 Potential of the Free Field on the Torus of Dimension at Most Two

Defines the Wick-ordered phi4phi^4 potential of the free field on the torus of dimension at most two as the pointwise limit of the Galerkin potentials along dyadic cutoffs, and zero where that limit does not exist.

Statement

In the settings of The Real Numbers: Standing Notation and Background and The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation, suppose n≤2n\le2, let ϰ,m∈R\varkappa,\mathfrak{m}\in\mathbb{R} with 0<ϰ0<\varkappa, and for N∈NN\in\mathbb{N} let VN:X→RV_{N}:X\to\mathbb{R} be the Galerkin Wick-ordered ϕ4\phi^{4} potential with cutoff NN, coupling ϰ\varkappa and mass m\mathfrak{m}; 2j2^{j} (j∈Nj\in\mathbb{N}) is the jj-th power of 22.

(The potential) The Wick-ordered ϕ4\phi^{4} potential of the free field on Tn\mathbb{T}^{n} with coupling ϰ\varkappa and mass m\mathfrak{m} is the function V:X→RV:X\to\mathbb{R} given, for x∈Xx\in X, by

V(x)=lim⁡j→∞V2j(x)if the real sequence (V2j(x))j∈N converges,V(x)=0otherwise.V(x)=\lim_{j\to\infty}V_{2^{j}}(x)\quad\text{if the real sequence }(V_{2^{j}}(x))_{j\in\mathbb{N}}\text{ converges},\qquad V(x)=0\quad\text{otherwise}.

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