The electron and positron annihilate to form a K⁰ (yellow ball), and a JET of particles such as pions (grey wedge). You can assume that the JET and the K⁰ each have a total energy equal to the Incident beam energy. The K⁰ travels in a straight line and leaves no track because it has zero electrical charge. After a period of time, usually short, the K⁰ decays into a  π+, π- pair (green and blue balls) its position of decay indicated by the white 'ghost' ball. The charged pion pair are affected by the uniform magnetic field, coming out of the screen, and follow curved trajectories.

As with the charged particle pairs in the previous exercise the K⁰ has no preferred direction of motion. Likewise the JET has no preferred direction, however, relative to the kaon it always points in the opposite direction in order to conserve momentum. Notice also that as the beam energy is increased the angular spread of the JET decreases.

Conservation of momentum causes the pions to be created travelling in the same general direction as the K⁰ was before it decayed. The pions also follow trajectories with different radii on each new firing sequence, since they have different momenta on each decay.

Despite changing on each firing sequence, the form of the pion trajectories fall into two main categories. Their tracks either, initially diverge before coming back on themselves and crossing, or they diverge and never cross (see Figure below). This is a consequence of the initial orientation of the π+, π- pair, at creation.