Experimentally, the NSCD requires the presence and proper orientation of the bulk magnetization of the nuclear spins (M). This magnetization emerges as the population average of individual nuclear magnetic moments and its evolution in time is the basis for nuclear magnetic resonance (NMR) spectroscopy. Since the presence of NSCD requires that this nuclear magnetization vector has a component parallel with the light beam, manipulating the direction of M is essential for the observation of NSCD. In other words, the time evolution of M will directly influence the time evolution of the NSCD.