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arXiv 1503.00897math-phmath.MP
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量子场论的变形与相互作用模型的建立

Deformations of Quantum Field Theories and the Construction of Interacting Models

Sabina Alazzawi

摘要:

本论文的主题是严格构造具有非平凡相互作用的QFT模型。AQFT框架中的两种不同的方法进行了讨论。一方面,考虑逆散射问题。一个给定的分解S-矩阵,从而采取作为建设的起点。考虑的粒子谱涉及任意数量的大质量粒子种类,在全球规范群下变换。从已知的楔形局部辅助领域,过渡到本地理论。为此,我们利用模核条件,并调查某些映射从楔形代数,所产生的辅助领域,所考虑的希尔伯特空间。根据一个非常合理的猜想,它表明,这些地图是核,这意味着非平凡的代数与有界区域的意义上,Reeh-Schlieder财产持有。用这种方法可以构造出一大类在1+1维上分解S-矩阵的可积模型。其中包括O(N)不变的非线性sigma模型。另一方面,形变技术构成了一种可以应用于任意时空维度的构造方法。这种方法从一个已知的量子场论模型,这是受到一定的修改。这里,具体地说,标量质量费米子的模型被变形了。新兴的模型是基于楔形局部场,允许计算的两个粒子的S-矩阵。所得到的散射矩阵取决于变形,并且不同于初始模型的散射矩阵。通过限制到1+1维,变形方法产生了一大类可积模型,其中包括Sinh-Gordon模型。

英文摘要:

The subject of this thesis is the rigorous construction of QFT models with nontrivial interaction. Two different approaches in the framework of AQFT are discussed. On the one hand, an inverse scattering problem is considered. A given factorizing S-matrix is thereby taken as the starting point of the construction. The particle spectrum taken into account involves an arbitrary number of massive particle species, transforming under a global gauge group. Starting from known wedge-local auxiliary fields, the transition to local theories is shown. To his end, we make use of the modular nuclearity condition and investigate certain maps from the wedge algebras, generated by the auxiliary fields, to the considered Hilbert space. Under a very plausible conjecture it is shown that these maps are nuclear, which implies the nontriviality of algebras associated with bounded regions in the sense that the Reeh-Schlieder property holds. A large class of integrable models with factorizing S-matrices in 1+1 dimensions can be constructed in this way. Among them are the O(N)-invariant nonlinear sigma-models. Deformation techniques, on the other hand, constitute a method of construction which may be applied in arbitrary spacetime dimensions. This approach starts from a known quantum field theoretic model which is subjected to a certain modification. Here, concretely, the model of a scalar massive Fermion was deformed. The emerging models are based on wedge-local fields, allowing for the computation of the two-particle S-matrix. The resulting scattering matrix depends on the deformation and differs from the one of the initial model. By restricting to 1+1 dimensions, the deformation method yields a large class of integrable models with factorizing S-matrices, including the Sinh-Gordon model.

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