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arXiv 2103.09328math-phmath.MP
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Lorentzian 符号下大质量 Sine-Gordon 理论的平衡态

Equilibrium states for the massive Sine-Gordon theory in the Lorentzian signature

Dorothea Bahns, Nicola Pinamonti, Kasia Rejzner

AI总结:

本文结合微扰代数量子场论与构造性量子场论技术,在二维 Minkowski 时空绝热极限下构造了大质量 Sine-Gordon 理论平衡态的关联函数,并证明了其幂级数在强算子拓扑下的收敛性及有限温度 KMS 态的可构造性。

摘要:

本文在二维 Minkowski 时空的热态中,研究了紫外有限区域内的大质量 Sine-Gordon 模型。我们结合近期发展的微扰代数量子场论方法与 Euclidean 时空上构造性量子场论领域的技术,在绝热极限下构造了 Sine-Gordon 理论平衡态的关联函数。首先,Sine-Gordon 理论的观测量被视为自由位形上的泛函,并通过将相互作用 Lagrange 量的 S-矩阵限制在自由大质量理论上的紧致时空区域中,经适当组合而获得。这些 S-矩阵以耦合常数的幂级数形式给出,其值属于自由大质量理论上的场代数。通过将条件化与逆条件化等技术适配到具有 Lorentzian 符号的时空中,我们证明了这些幂级数在一般场位形上求值时是收敛的。后一观察意味着在所考虑态的 GNS 表示中,强算子拓扑下的收敛性。在论文第二部分,通过将集团展开技术适配到 Lorentzian 情形,我们证明了在绝热极限下,有限温度下相互作用平衡态(KMS 态)的关联函数同样可以被构造,此时相互作用 Lagrange 量在空间各处均有支撑。

英文摘要:

In this paper we investigate the massive Sine-Gordon model in the ultraviolet finite regime in thermal states over the two-dimensional Minkowski spacetime. We combine recently developed methods of perturbative algebraic quantum field theory with techniques developed in the realm of constructive quantum field theory over Euclidean spacetimes to construct the correlation functions of the equilibrium state of the Sine-Gordon theory in the adiabatic limit. First of all, the observables of the Sine-Gordon theory are seen as functionals over the free configurations and are obtained as a suitable combination of the S-matrices of the interaction Lagrangian restricted to compact spacetime regions over the free massive theory. These S-matrices are given as power series in the coupling constant with values in the algebra of fields over the free massive theory. Adapting techniques like conditioning and inverse conditioning to spacetimes with Lorentzian signature, we prove that these power series converge when evaluated on a generic field configuration. The latter observation implies convergence in the strong operator topology in the GNS representations of the considered states. In the second part of the paper, adapting the cluster expansion technique to the Lorentzian case, we prove that the correlation functions of the interacting equilibrium state at finite temperature (KMS state) can be constructed also in the adiabatic limit, where the interaction Lagrangian is supported everywhere in space.

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