{"title":"The massless S-matrix of integrable $σ$-models","authors":"George Georgiou","doi":"arxiv-2408.03673","DOIUrl":null,"url":null,"abstract":"In contradistinction to the case of massive excitations, the connection\nbetween integrability and the tree-level massless scattering matrix of\nintegrable $\\sigma$-models is lost. Namely, in well-known 2-d integrable models\nthe tree-level massless S-matrix exhibits particle production and fails to\nfactorise. This is conjectured to happen due to IR ambiguities in the massless\ntree-level amplitudes. We present a definition of the massless S-matrix which\nhas all the nice properties of integrable theories, there is no particle\nproduction and the S-matrix factorises. As an example, we present in detail the\ncase of the $SU(2)$ principal chiral model (PCM).","PeriodicalId":501592,"journal":{"name":"arXiv - PHYS - Exactly Solvable and Integrable Systems","volume":"6 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Exactly Solvable and Integrable Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.03673","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In contradistinction to the case of massive excitations, the connection
between integrability and the tree-level massless scattering matrix of
integrable $\sigma$-models is lost. Namely, in well-known 2-d integrable models
the tree-level massless S-matrix exhibits particle production and fails to
factorise. This is conjectured to happen due to IR ambiguities in the massless
tree-level amplitudes. We present a definition of the massless S-matrix which
has all the nice properties of integrable theories, there is no particle
production and the S-matrix factorises. As an example, we present in detail the
case of the $SU(2)$ principal chiral model (PCM).
与大质量激元的情况相反,可积分性与可积分的$\sigma$模型的树级无质量散射矩阵之间失去了联系。也就是说,在著名的二维可积分模型中,树级无质量S矩阵表现出粒子产生,而无法因子化。据推测,这是由于质量树级振幅的红外模糊性造成的。我们提出了无质量 S 矩阵的定义,它具有可积分理论的所有优良特性,不存在粒子产 生,而且 S 矩阵能够因式分解。作为一个例子,我们详细介绍了$SU(2)$主手性模型(PCM)的情况。