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Lambda-nucleon scattering in baryon chiral perturbation theory

机译:Baryon手术扰动理论中的Lambda核心散射

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摘要

We calculate the Lambda-nucleon scattering phase shifts and mixing angles by applying time-ordered perturbation theory to the manifestly Lorentz-invariant formulation of SU(3) baryon chiral perturbation theory. Scattering amplitudes are obtained by solving the corresponding coupled-channel integral equations that have a milder ultraviolet behavior compared to their nonrelativistic analogs. This allows us to consider the removed cutoff limit in our leading-order calculations also in the P-3(0) and P-3(1) partial waves. We find that, in the framework we are using, at least some part of the higher-order contributions to the baryon-baryon potential in these channels needs to be treated nonperturbatively, and we demonstrate how this can be achieved in a way consistent with quantum field theoretical renormalization for the leading contact interactions. We compare our results with the ones of the nonrelativistic approach and lattice QCD phase shifts obtained for non-physical pion masses.
机译:我们通过将时间顺序的扰动理论施加到明显的Lorentz-Fonorboration理论的明显洛伦兹 - 不变制剂来计算Lambda-Nucleors散射相移和混合角度。 通过求解与它们的非椭圆形类似物相比具有更温和的紫外线行为的相应耦合通道整体方程来获得散射幅度。 这允许我们考虑我们的领先顺序计算中的除去截止限制,也在P-3(0)和P-3(1)部分波中。 我们发现,在我们使用的框架中,至少对这些渠道中的Baryon-Baryon电位的至少一些部分需要进行非耐受,并且我们证明了如何以与量子一致的方式实现这一目标 领域的理论重整化对领先的接触相互作用。 我们将我们的结果与非物理π块的非椭圆形方法和晶格QCD相移进行比较。

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