Abstract
Using a two-body separable $t$ matrix between pairs, we solve the resulting four-body equations for four spinless bosons in the form that the 2+2 subsystem contribution is treated exactly by the convolution method. The 3+1 subamplitudes are represented as finite rank operators. We compare the utility of these methods both in four-body bound state and scattering calculations. We also develop an approximation that neglects four-body intermediate states in the 2+2 subsystem contribution and compare it with exact results. Finally, we present the results for a four-nucleon calculation with spin dependent $s$-wave separable interactions between pairs. These formally exact four-body equations are subsequently used to develop one parameter models to describe low energy phase shifts and cross sections for the reactions n $^{3}\mathrm{H}$\ensuremath{\rightarrow}n $^{3}\mathrm{H}$, dd\ensuremath{\rightarrow}dd, and dd\ensuremath{\rightarrow}p $^{3}\mathrm{H}$.
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