Let us introduce a fictitious particle called spurion of I = 1/2, I3 = −1/2, and neutrally charged and add it on the left hand side so that the weak decay is converted into a strong interaction in which I is conserved. The reactions with Σ+ can proceed in I = 1/2 and 3/2 channels while that with Σ− through pure I = 3/2 channel. We can then write down the amplitudes for the initial state by referring to the C.G. coefficients for 1 × 1/2: