Again, here we have two possible Feynman diagrams, Figs. $4.5$ a and $4.5 \mathrm{c}$. We are working only in terms of particle (electron) states, and so we must use the antiparticle prescription, (3.28), to translate these to diagrams (b) and (d), respectively. We can use the Feynman rules (obtained above and collected in Section 6.17) to calculate the (lowest-order) $\mathrm{e}^{-} \mathrm{e}^{+} \rightarrow \mathrm{e}^{-} \mathrm{e}^{+}$amplitude