I=3/2Nπ scattering and the ∆(1232) resonance on $N_f=2+1$ CLS ensembles using the stochastic LapH method

C. Andersen, J. Bulava, Ben Horz, C. Morningstar
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引用次数: 3

Abstract

Calculations of the elastic $I=\frac{3}{2}$ nucleon-pion scattering phase shifts on two lattice QCD ensembles with $m_\pi=200\mathrm{MeV}$ and $280\mathrm{MeV}$ are presented. The ensembles both employ $N_\mathrm{f} = 2+1$ Wilson clover fermions. We determine the $\Delta(1232)$ resonance parameters from a finite volume scattering analysis. In one study the single partial wave simplification is employed to compute the $p$-wave amplitude while in the other we treat the partial wave mixing between $s$- and $p$-wave contributions. Fitting our data to a Breit-Wigner resonance model we find $m_\Delta/m_\pi = 7.13(9)$ and $4.75(5)$ on the two ensembles respectively, showing that for a lighter quark mass the resonance mass moves from near the $N\pi$ threshold to near the $N\pi\pi$ threshold, in agreement with experiment.
用随机LapH方法研究$N_f=2+1$ CLS系综上I=3/2Nπ散射和∆(1232)共振
给出了两个具有$m_\pi=200\mathrm{MeV}$和$280\mathrm{MeV}$的晶格QCD系综上弹性$I=\frac{3}{2}$核子-介子散射相移的计算。合奏都使用$N_\mathrm{f} = 2+1$威尔逊三叶草费米子。我们从有限体积散射分析中确定$\Delta(1232)$共振参数。在一项研究中,采用单部分波简化来计算$p$ -波振幅,而在另一项研究中,我们处理$s$ -波和$p$ -波贡献之间的部分波混频。将我们的数据拟合到Breit-Wigner共振模型中,我们分别在两个系综上找到$m_\Delta/m_\pi = 7.13(9)$和$4.75(5)$,表明对于较轻的夸克质量,共振质量从$N\pi$阈值附近移动到$N\pi\pi$阈值附近,与实验一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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