“…Figure 2: Graphical representation of a configuration representing contributions to the total momentum for a system at rest due to momenta, p 1 and p 2 , of particles 1 and 2, and to the interaction part, (2 m/M)Ṽ u. It is reminded that the two contributions, which sum up here to zero, separately cancel in an earlier implementation of the point-form approach [2,3,4]. Contrary to the front-form approach, the interaction part and, consequently, the sum of the particle momenta, p 1 + p 2 , points isotropically to all directions, which is sketched by circles for the momentum configuration drawn in the figure.…”