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Reflection-Symmetric Periodic Pair Interactions on the Lattice Torus, Their Interaction Matrices and Their Symbols

A reflection-symmetric periodic pair interaction is a function on the integer lattice that is periodic with period L and invariant under each coordinate reflection. Its interaction matrix couples two sites through their difference, and its symbol is its cosine transform over one period.

Statement

In the settings of The Real Numbers: Standing Notation and Background and The Flat Torus: Standing Notation, with the dimension nn, the initial segment [n][n] and the integer lattice Zn\mathbb{Z}^{n}, let M∈NM\in\mathbb{N}, and let the side L=2M+1L=2M+1, the cube ΓM\Gamma_{M}, the set WLW_{L} and the lattice torus LM\mathbb{L}_{M} be those of The Lattice Torus of Odd Side, Lattice Fields, and the Discrete Fourier Coefficients of a Lattice Field. For m∈Zm\in\mathbb{Z}, Cm:R→RC_{m}:\mathbb{R}\to\mathbb{R} is the trigonometric monomial Cm(t)=cos⁡(2πmt)C_{m}(t)=\cos(2\pi mt) of Cell Integrals of the Trigonometric Monomials. Finite products of real numbers indexed by [n][n] are those of Finite Product Notation in a Field, and sums over finite index sets those of Sum over a Finite Index Set. For i∈[n]i\in[n], Ri:Zn→ZnR_{i}:\mathbb{Z}^{n}\to\mathbb{Z}^{n} is the map changing the sign of the ii-th component and keeping the others.

1. (Interaction) A reflection-symmetric periodic pair interaction of side LL is a map j:Zn→R\mathfrak{j}:\mathbb{Z}^{n}\to\mathbb{R} such that

j(w+Ll)=j(w)andj(Riw)=j(w)for all w,l∈Zn and i∈[n].\mathfrak{j}(w+Ll)=\mathfrak{j}(w)\qquad\text{and}\qquad\mathfrak{j}(R_{i}w)=\mathfrak{j}(w)\qquad\text{for all }w,l\in\mathbb{Z}^{n}\text{ and }i\in[n].

2. (Interaction matrix) The interaction matrix of a reflection-symmetric periodic pair interaction j\mathfrak{j} of side LL is the map J:LM×LM→RJ:\mathbb{L}_{M}\times\mathbb{L}_{M}\to\mathbb{R}, J(y,z)=j(L(y−z))J(y,z)=\mathfrak{j}\bigl(L(y-z)\bigr). Here L(y−z)=w−w′∈ZnL(y-z)=w-w'\in\mathbb{Z}^{n} for y=L−1wy=L^{-1}w and z=L−1w′z=L^{-1}w' with w,w′∈WLw,w'\in W_{L}, and every site is of this form by The Lattice Torus of Odd Side, Lattice Fields, and the Discrete Fourier Coefficients of a Lattice Field §lattice.

3. (Symbol) The symbol of j\mathfrak{j} is the map J^:ΓM→R\hat{J}:\Gamma_{M}\to\mathbb{R},

J^(k)=∑w∈WLj(w)∏i=1nCki(L−1wi)(k∈ΓM),\hat{J}(k)=\sum_{w\in W_{L}}\mathfrak{j}(w)\prod_{i=1}^{n}C_{k_{i}}\bigl(L^{-1}w_{i}\bigr)\qquad(k\in\Gamma_{M}),

a sum of real numbers over the nonempty finite set WLW_{L} of The Lattice Torus of Odd Side, Lattice Fields, and the Discrete Fourier Coefficients of a Lattice Field §lattice, the product being over [n][n] with ki∈Zk_{i}\in\mathbb{Z}.

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