“…In fact, one can perform the Feynman-diagrammatic computation only for the partial amplitudes which are independent under crossings of the external momenta and obtain the rest only at the end. For the processes above, this means one can restrict the computation to just A [1] 4𝑔 , A [4] 4𝑔 , A [1] 𝑞𝑔 , A [3] 𝑞𝑔 , A [1] 4𝑞 , A [2] 4𝑞 . In order to compute the set of independent partial amplitudes, we further decompose them in Lorentz (or spin) space.…”