Standard Model and Beyond · Problem 2.10

Lie Groups, Lie Algebras, and Symmetries

Physics — Particle Physics · gordon-decomposition

Problem

Prove the Gordon decomposition formulas 2m(uˉ2γμu1)=uˉ2(p2+p1)μu1+iuˉ2σμν(p2−p1)νu12m(uˉ2γμγ5u1)=uˉ2(p2−p1)μγ5u1+iuˉ2σμν(p2+p1)νγ5u10=uˉ2(p2−p1)μu1+iuˉ2σμν(p2+p1)νu10=uˉ2(p2+p1)μγ5u1+iuˉ2σμν(p2−p1)νγ5u1,\begin{aligned} 2m(\bar{u}_2\gamma^\mu u_1) &= \bar{u}_2(p_2+p_1)^\mu u_1 + i\bar{u}_2\sigma^{\mu\nu}(p_2-p_1)_\nu u_1\\ 2m(\bar{u}_2\gamma^\mu\gamma^5 u_1) &= \bar{u}_2(p_2-p_1)^\mu\gamma^5 u_1 + i\bar{u}_2\sigma^{\mu\nu}(p_2+p_1)_\nu\gamma^5 u_1\\ 0 &= \bar{u}_2(p_2-p_1)^\mu u_1 + i\bar{u}_2\sigma^{\mu\nu}(p_2+p_1)_\nu u_1\\ 0 &= \bar{u}_2(p_2+p_1)^\mu\gamma^5 u_1 + i\bar{u}_2\sigma^{\mu\nu}(p_2-p_1)_\nu\gamma^5 u_1, \end{aligned} where u1,2u_{1,2} are two Dirac uu spinors for a particle of mass mm.

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