Abstract
The Alt, Grassberger, and Sandhas four-body theory has been used to calculate the differential cross sections for the kinematically complete breakup reaction $^{3}\mathrm{He}$(p,pd${)}^{1}$H at various proton energies and angles. The two-body input consists of Yamaguchi potentials without Coulomb corrections and the (3+1) and (2+2) amplitudes were expanded using the generalized unitary pole expansion. The resulting effective two-body equations have been solved in the first-order K-matrix approximation. Reasonable agreement with experiment was obtained.
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