{"title":"Three-particle formalism for multiple channels: the $ηππ+ K \\overline K π$ system in isosymmetric QCD","authors":"Zachary T. Draper, Stephen R. Sharpe","doi":"arxiv-2403.20064","DOIUrl":null,"url":null,"abstract":"We generalize previous three-particle finite-volume formalisms to allow for\nmultiple three-particle channels. For definiteness, we focus on the two-channel\n$\\eta \\pi \\pi$ and $K \\overline K \\pi$ system in isosymmetric QCD, considering\nthe positive $G$ parity sector of the latter channel, and neglecting the\ncoupling to modes with four or more particles. The formalism we obtain is thus\nappropriate to study the $b_1(1235)$ and $\\eta(1295)$ resonances. The\nderivation is made in the generic relativistic field theory approach using the\ntime-ordered perturbation theory method. We study how the resulting\nquantization condition reduces to that for a single three-particle channel when\none drops below the upper ($K\\overline K \\pi$) threshold. We also present\nparametrizations of the three-particle K matrices that enter into the\nformalism.","PeriodicalId":501191,"journal":{"name":"arXiv - PHYS - High Energy Physics - Lattice","volume":"53 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-03-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Lattice","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2403.20064","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
We generalize previous three-particle finite-volume formalisms to allow for
multiple three-particle channels. For definiteness, we focus on the two-channel
$\eta \pi \pi$ and $K \overline K \pi$ system in isosymmetric QCD, considering
the positive $G$ parity sector of the latter channel, and neglecting the
coupling to modes with four or more particles. The formalism we obtain is thus
appropriate to study the $b_1(1235)$ and $\eta(1295)$ resonances. The
derivation is made in the generic relativistic field theory approach using the
time-ordered perturbation theory method. We study how the resulting
quantization condition reduces to that for a single three-particle channel when
one drops below the upper ($K\overline K \pi$) threshold. We also present
parametrizations of the three-particle K matrices that enter into the
formalism.
我们概括了以前的三粒子有限体积形式主义,以允许多个三粒子通道。为了明确起见,我们重点研究了等对称QCD中的双通道$\eta \pi \pi$和$K \overline K \pi$系统,考虑了后一通道的正$G$奇偶性扇区,并忽略了与四或更多粒子模式的耦合。因此,我们得到的形式主义适合于研究$b_1(1235)$和$\ea(1295)$共振。我们使用时序扰动理论方法,在一般相对论场论方法中进行了衍生。我们研究了当一个粒子降到上阈值($K\overline K \pi$)以下时,所产生的量子化条件如何降低到单个三粒子通道的量子化条件。我们还提出了进入形式主义的三粒子 K 矩阵的参数化。