In view of the recent results of lattice QCD simulation in the P11 partialwave that has found no clear signal for the three-quark Roper state weinvestigate a different mechanism for the formation of the Roper resonance in acoupled channel approach including the $\pi N$, $\pi\Delta$ and $\sigma N$channels. We fix the pion-baryon vertices in the underlying quark model whilethe s-wave sigma-baryon interaction is introduced phenomenologically with thecoupling strength, the mass and the width of the $\sigma$ meson as freeparameters.The Laurent-Pietarinen expansion is used to extract the informationabout the $S$-matrix pole. The Lippmann-Schwinger equation for the $K$ matrixwith a separable kernel is solved to all orders. For sufficiently strong$\sigma NN$ coupling the kernel becomes singular and a quasi-bound stateemerges at around 1.4 GeV, dominated by the $\sigma N$ component and reflectingitself in a pole of the $S$-matrix. The alternative mechanism involving a$(1s)^22s$ quark resonant state is added to the model and the interplay of thedynamically generated state and the three-quark resonant state is studied. Itturns out that for the mass of the three-quark resonant state above 1.6 GeV themass of the resonance is determined solely by the dynamically generated state,nonetheless, the inclusion of the three-quark resonant state is imperative toreproduce the experimental width and the modulus of the resonance pole.
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机译:鉴于最近在P11子波中进行晶格QCD模拟的结果尚未发现三夸克Roper态的清晰信号,我们研究了在耦合通道方法中形成Roper共振的另一种机制,包括$ \ pi N $, $ \ pi \ Delta $和$ \ sigma N $个通道。我们将pion-baryon顶点固定在基本的夸克模型中,而s波sigma-baryon相互作用是从现象学上引入的,耦合强度,$ \ sigma $介子的耦合强度,质量和宽度作为自由参数.Laurent-Pietarinen展开用于提取有关$ S $-矩阵极的信息。将具有可分离核的$ K $矩阵的Lippmann-Schwinger方程求解为所有阶数。对于足够强的$ \ sigma NN $耦合,内核变为奇异,准绑定状态在1.4 GeV处出现,由$ \ sigma N $分量主导,并在$ S $矩阵的一个极点中反映出来。在模型中加入了一个涉及($ 1s)^ 22s $夸克共振态的替代机制,研究了动态生成态与三夸克共振态的相互作用。结果表明,对于高于1.6 GeV的三夸克共振态的质量,共振的质量仅由动态产生的状态决定,尽管如此,必须包含三夸克共振态以重现实验宽度和模量。共振极。
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