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arXiv 1111.2547hep-thmath-phmath.MP
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sinh-和sine-Gordon模型的共振和Liouville理论中的高级运动方程

Resonances in sinh- and sine-Gordon models and higher equations of motion in Liouville theory

Michael Lashkevich

摘要:

算子共振的概念是由扎莫洛奇科夫在共形微扰理论的框架内提出的。共振与微扰展开中积分的对数发散有关,并表现在关联函数的极点和局部算子的形状因子中,它们被认为是共形维数的函数。极点的留数可以用一些算子恒等式来计算。在这里,我们研究的共振刘维尔,sinh和正弦戈登模型,被认为是一个无质量的自由玻色子的扰动。我们证明了由Al. Zamolodchikov在Liouville场论中发现的著名的高阶运动方程只不过是某些后代算子的共振恒等式。共振点附近的共振展开提供了相应算子的正则化版本。我们试图在sinh-和sine-Gordon理论中构造相应的共振恒等式和共振展开式。在某些情况下,它可以显式地完成,但在大多数情况下,到目前为止,我们只能获得一般形式。然而,我们表明,共振是微扰精确的,这意味着他们中的每一个只出现在一个单一的术语的微扰理论。

英文摘要:

The notion of operator resonances was introduced earlier by Al. Zamolodchikov within the framework of the conformal perturbation theory. The resonances are related to logarithmic divergences of integrals in the perturbation expansion, and manifest themselves in poles of the correlation functions and form factors of local operators considered as functions of conformal dimensions. The residues of the poles can be computed by means of some operator identities. Here we study the resonances in the Liouville, sinh- and sine-Gordon models, considered as perturbations of a massless free boson. We show that the well-known higher equations of motion discovered by Al. Zamolodchikov in the Liouville field theory are nothing but resonance identities for some descendant operators. The resonance expansion in the vicinity of a resonance point provides a regularized version of the corresponding operators. We try to construct the corresponding resonance identities and resonance expansions in the sinh- and sine-Gordon theories. In some cases it can be done explicitly, but in most cases we are only able to obtain a general form so far. We show nevertheless that the resonances are perturbatively exact, which means that each of them only appears in a single term of the perturbation theory.

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