Direct construction of scalar quantum fields by L{é}vy fields -- nontrivial exact Wightman fields in a wider field with a relaxed Gårding-Wightman Axioms-

Abstract

This paper introduces partial results, in the current situation, of ongoing considerations corresponding to the above title. A construction on exact relativistic quantum field model with the space time dimension $d\in \mathbb{N}$, including the case where $d\ge 4$, is going to be discussed. Firstly, Hermitian scalar quantum fields $<\mathcal{H},U,\psi ,D>$, within a relaxed framework of the Gårding-Wightman Axioms, is constructed by making use of the stochastic calculus arguments with respect to the {\it{stationary additive random fields }} on ${\mathbb{R}}^d$, i.e., the {\it{L{é}vy random fields}} on ${\mathbb{R}}^d$. The first constructed $<\mathcal{H},U,\psi ,D>$, here, satisfy all the requirements of the the Gårding-Wightman Axioms, except that the field operators $\psi (f)$ with $f\in \mathcal{S}({\mathbb{R}}^d\to \mathbb{R})$ are symmetric operators on the physical Hilbert space $\mathcal{H}$, which situation is denoted here as {\it{a relaxed framework}} of the Gårding-Wightman Axioms. Secondly, by taking the adequate subspaces of $\mathcal{H}$, non trivial exact Wightman quantum fields, which satisfy all the requirements of the Gårding-Wightman Axioms, are constructed actually. keywords: Axiomatic quantum field theory, Gårding-Wightman axioms, Bochner-Minlos theorem, L{é}vy fields on ${\mathbb{R}}^d$.