$T\bar{T}$ 变形:一种晶格方法

Yunfeng Jiang
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引用次数: 0

摘要

可积分量子场论可以在保留可积分性的同时在晶格上正则化。由此产生的晶格理论是可积分的晶格模型。这种正则化的一个原型是正弦-戈登模型与光锥晶格上的 6 顶点模型之间的对应关系。我们提出了光锥晶格模型的可积分变形,这样在连续极限中我们就得到了$T\bar{T}$变形的正弦-戈登模型。在这种变形下,截止动量变得与能量有关,而基本的杨-巴克斯特可积分性却得以保留。因此,这种变形是可积分但非局部的,类似于量子场论的$T\bar{T}$ 变形。
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$T\bar{T}$-deformation: a lattice approach
Integrable quantum field theories can be regularized on the lattice while preserving integrability. The resulting theory on the lattice are integrable lattice models. A prototype of such a regularization is the correspondence between sine-Gordon model and 6-vertex model on a light-cone lattice. We propose an integrable deformation of the light-cone lattice model such that in the continuum limit we obtain the $T\bar{T}$-deformed sine-Gordon model. Under this deformation, the cut-off momentum becomes energy dependent while the underlying Yang-Baxter integrability is preserved. Therefore this deformation is integrable but non-local, similar to the $T\bar{T}$-deformation of quantum field theory.
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