“…In fact, our operator has the structure λβργ G µα (z)G ργ (0), where G(z) and G(0) is the same field. As we will see in section 2.5, this imposes two relations (2.28), (2.33) between some invariant amplitudes M parametrizing M (2) µα;λβ and invariant amplitudes entering into M (1) µα;λβ . One may also incorporate the symmetry properties of M µα;λβ (z, p) with respect to z. Namely, since M µα;λβ (z, p) is odd in z, the invariant amplitudes M sp , M ps , M pzsz , M szpz , M zp , M pz are odd functions of ν, while the remaining ones are even functions of ν.…”