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D-state configurations in the electromagnetic form factors of the nucleon and the Delta(1232) resonance

机译:D状态配置中的电磁形状因子   核子和Delta(1232)共振

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摘要

The $\Delta-N$ electromagnetic transition form factors are calculated in thePoincar\'e covariant quark model in three forms of relativistic kinematics.Addition of $D-$state components to pure $S-$state model wave functions, chosenso as to reproduce the empirical elastic electromagnetic nucleon form factorswith single constituent currents, brings the calculated $R_{EM}$ ratio for the$\Delta(1232)\to N\gamma$ transition closer to the empirical values in instantand point form kinematics. The calculated $R_{SM}$ ratio is insensitive to the$D-$state component. In front form kinematics the substantial violation of theangular condition for the spin 3/2 resonance transition amplitude in theimpulse approximation prevents a unique determination of $R_{EM}$ and $R_{SM}$,both of which are very sensitive to $D-$state components. In no form ofkinematics do $D-$state deformations of the rest frame baryon wave functionsalone suffice for a description of the empirical values of these ratios.
机译:在庞加莱协变夸克模型中以相对论运动学的三种形式计算$ \ Delta-N $电磁跃迁形状因数,将$ D- $ state分量添加到纯$ S- $ state模型波动函数中,选择用单个成分电流重现经验弹性电磁核子形状因数,使计算出的Δ(Delta(1232)\)到N \γ$跃迁的$ R_ {EM} $比值更接近瞬时和点形式运动学中的经验值。计算得出的$ R_ {SM} $比率对$ D- $ state分量不敏感。在前形式运动学中,在脉冲近似中对自旋3/2共振跃迁幅度的角度条件的严重违反使$ R_ {EM} $和$ R_ {SM} $的唯一确定无法确定,这两者对$ D非常敏感-$ state组件。在任何形式的运动学中,静止帧重子波函数的$ D- $ state变形都不能单独描述这些比率的经验值。

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