A study of nucleon-nucleon scattering in covariant chiral effective field theory at the two-loop level
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摘要: 从协变手征有效理论出发, 计算了核子-核子(Nucleon-Nucleon, N-N)散射两圈图振幅. 两圈图是以箱图为骨架并对π介子自能进行修正所得. 在减除时, 采用两种减除方案:
$\overline {{\rm{MS}}}$ 和${\rm{E}}\overline {{\rm{MS}}} \left( {{\rm{Extended}}\;\overline {{\rm{MS}}} } \right)$ . 由$\overline {{\rm{MS}}}$ 得到的振幅严重破坏手征微扰展开的幂次规则, 由${\rm{E}}\overline {{\rm{MS}}}$ 得到的振幅中仅余非定域“反常”贡献, 剩下的均是满足手征幂次规则的贡献.Abstract: The amplitude of the two-loop level in N-N(nucleon-nucleon) scattering is calculated using covariant chiral effective theory. Based on the skeleton of the box diagram, the two-loop diagram results from the correction of pion self-energy. Two subtraction schemes will be employed for comparison:$\overline {{\rm{MS}}}$ and${\rm{E}}\overline {{\rm{MS}}}$ . The loop amplitude obtained with$\overline {{\rm{MS}}}$ contains terms that violate chiral power counting rules; with${\rm{E}}\overline {{\rm{MS}}}$ , the results are entirely chiral contributions with the exception of non-local “anomalous” ones that must be retained. -
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