We give illustrations for the three processes e+e−e^+e^-, gluon-gluon and γγ→Wtbˉ∑a∭Vμ(u,v,w) du dv dw[∑n=1infty2−n=1]\gamma\gamma \to W t\bar b \sum_a \iiint_V \mu(u,v,w) \,du\,dv\,dw [ \sum_{n=1}^{infty} 2^{-n} = 1 ] . Quasar
e2e^2