TheoremBase

The Gradient Energy with a Mode Cutoff

At cutoff N the gradient energy of a function at a state is the sum over the kept modes of its squared first mode derivatives; the uncut gradient energy is the limit in N where it exists.

Statement

In the setting of The Wick-Square Problem on the Torus: Standing Notation, let φ:H−1→R\varphi:H^{-1}\to\mathbb{R} be twice differentiable along the modes, with first mode derivatives ∂kφ\partial_{k}\varphi, and let x∈H−1x\in H^{-1}. Sums over the cube ΓN\Gamma_{N} are sums over a finite index set.

1. (At cutoff NN) For N∈NN\in\mathbb{N}, the gradient energy at cutoff NN of φ\varphi at xx is

∣DNφ(x)∣2=∑k∈ΓN(∂kφ(x))2.|D_{N}\varphi(x)|^{2}=\sum_{k\in\Gamma_{N}}\bigl(\partial_{k}\varphi(x)\bigr)^{2}.

2. (Uncut) If the sequence (∣DNφ(x)∣2)N∈N(|D_{N}\varphi(x)|^{2})_{N\in\mathbb{N}} converges, ∣Dφ(x)∣2|D\varphi(x)|^{2} is said to be defined, and denotes the limit, which is unique by claim 1 of Uniqueness of Limits and Boundedness of Convergent Real Sequences.

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