Now let's look at the problem of dipole electric moment of elementary particles. Suppose that elementary force has an electric dipole moment. Then, based on what was said above (see g. 0), this vector should be oriented to the specific spin vector
0, i.e.:
d =t0 (0.00) If the system has symmetric symmetry, then if x, y, z coordinates are replaced by -x, -y, -z coordinates
(0.00) relation is not preserved. However, since d = ei and
s = [pr]=
t], tr0-x,-y,-z) = -d(x,y,z)
",[#
and S(-x,-y,-z) = S(x,y,z), so K = 0 and d = 0.
But in this case, the opposite is not true. that
K=0 because of conservation of frequency and invariance of time (t+-t). Also, when t-+-t changes: d(-t) = d(t) and
S(-t; = -d(t) in this case K=0.
Thus, the electric dipole moment of the system is simultaneously