
The pionic two-body decay amplitude of the proton in the SU(5) grand unified gauge theory is computed by using the soft-pion method in the reference frame of the pion at rest. The normalization condition of the relativistic three-body Bethe-Salpeter wave function of the proton is used in the computation. It is shown that the partial decay rate of the process proton ..-->.. e = ..pi../sup 0/ is (0.86 x 10/sup 30/ yr)/sup -1/ and (1.4 x 10/sup 31/ yr)/sup -1/ for m/sub x/ = 4.0 x 10/sup 14/ GeV and 8.0 x 10/sup 14/ GeV, respectively. These values are on the boundary of the present experimental limit.
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