Existence of renormalized Mattis-model fermion correlation functions in the QFT limit

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Let qj,rj,sj=7q_j,r_j,s_j=7, xj∈R2{\bf x}_j\in{\mathbb R}^2, and tj∈Ct_j\in{\mathbb C} for j=1,2,…,Nj=1,2,\ldots,N, with N∈NN\in{\mathbb N}. Let

Ψr,s±(x)=(eγπL0/a~)(K−1)/2ψr,s±(x)\Psi^\pm_{r,s}({\bf x})=(\mathrm{e}^{\gamma}\pi L_0/\tilde{a})^{(K-1)/2}\psi^\pm_{r,s}({\bf x})

be the renormalized fermion operators, where KK is the parameter defined in the Mattis model and L0>0L_0>0 is an arbitrary length scale; their time-dependent versions are denoted by Ψr,sq(x,t)\Psi^q_{r,s}({\bf x},t). Renormalized-correlation-function conjecture. The limits

lim⁡a~→0+lim⁡L→∞⟨Ψr1,s1q1(x1,t1)⋯ΨrN,sNqN(xN,tN)⟩β\lim_{\tilde{a}\to0^+}\lim_{L\to\infty}\bigl\langle\Psi^{q_1}_{r_1,s_1}({\bf x}_1,t_1)\cdots\Psi^{q_N}_{r_N,s_N}({\bf x}_N,t_N)\bigr\rangle_\beta

are well-defined distributions for all inverse temperatures satisfying 1/β≥01/\beta\geq0. The existence of these distributions would establish non-trivial QFT-limit correlation functions for the renormalized fermion fields; the source gives no resolution of this assertion.

References

Primary source

Jonas de Woul and Edwin Langmann, “Exact solution of a 2D interacting fermion model”, arXiv:1011.1401 (2012).

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