Show, by using particle helicities, that high-energy Compton scattering via the first diagram of Fig. 6.12 is, in the center-of-mass frame, given by
$$
\begin{aligned}
& \left.\left|\overline{\left.R_1\right|^2} \propto\right| d_{++}^{1 / 2}(\theta)\right|^2+\left|d^{1 / 2}(\theta)\right|^2 \\
& =(1+\cos \theta) \simeq-\frac{u}{2 s}, \\
&
\end{aligned}
$$
in agreement with (6.112). An example of this type of calculation is described in Section 6.6.