Figure 7

Left: $B_2$ as a function of $\pt$ /A for d (filled circles) ,$^3$He (empty circles) , and $^{3}_{\Lambda}\rm{H}$ (filled squares). The $B_2^{(\mathrm{d},^{3}_{\Lambda}\mathrm{H})}$ and $B_2^{(\mathrm{d}, ^{3}\mathrm{He})}$ were evaluated as explained in the text. k$_1 = \frac{m_\mathrm{d}^2}{m_{^{3}\mathrm{He}}m_{\mathrm{p}}}$,and k$_2 = \frac{m_\mathrm{d}^2 m_{\Lambda}}{m_{\mathrm{p}}^2 m_{^{3}_{\Lambda}\mathrm H}}$ Right: $S_{3}$ ratio measured in this analysis compared with previous experimental results (E864 and STAR (triangle and star, respectively)) and different theoretical models as indicated in the legend.