Figure 1

Nucleon analyzing power $A_y(N)$ and deuteron analyzing power $T_{21}$ for $\mathit{pd}$ elastic scattering at 3 MeV proton lab energy as functions of the c.m. scattering angle. The results of the two new calculational schemes without perturbation theory are graphically indistinguishable and are therefore represented by one curve only, the thin solid one; they are compared with the results obtained using perturbative approach of Refs. 1, 2 (thick dotted curves). Results without Coulomb (dashed curves) are given as reference for the size of the Coulomb effect.Reuse & Permissions

Figure 2

Differential cross section and deuteron analyzing power $A_{\mathit{xx}}$ for $\mathit{pd}$ breakup at 130 MeV deuteron lab energy in the kinematical configuration $({15}^{°},{15}^{°},{160}^{°})$ are shown as functions of the arclength $S$ along the kinematical curve. Curves as in Fig. 1.Reuse & Permissions