  But the z-spin disposition of the R-particle changes immediately after an (earlier) z-spin measurement on the L-particle: The R-particles 1-3 (see Fig. 4), which were previously disposed to z-spin ‘up,’ will now be disposed to z-spin ‘down,’ i.e., to emerge below the center plane aligned orthogonally to the z-axis; and the R-particles 4-6, which were previously disposed to z-spin ‘down,’ will now be disposed to z-spin ‘up,’ i.e., to emerge above this center plane. Yet, the L-measurement per se does not have any immediate influence on the state of the R-particle: The L-measurement does not influence the position of the R-particle or any other property that is directly derived from this position. It only changes the guiding field, and thus grounds new spin dispositions for the R-particle. But these dispositions are not intrinsic properties of the R-particle. Rather, they are relational properties of the R-particle, which are grounded in the positions of both particles and the state of the guiding  field.[17]  (Note that in the particular case in which the L-particle is emitted above the center plane aligned orthogonally to the z-axis and the R-particle is emitted below that plane, an earlier z-spin on the L-particle will have no influence on the outcome of a z-spin on the R-particle.)