This corresponds to the original definition of d orbitals with
L=2 and
m=-2,-1,0,1,2
The symmetry of the states expressed in the form of transformation in terms of x,y and z is shown in the table.
Isotropic potential | m=0 zz | m=1 xz+iyz | m=-1 xz-iyz | m=2 xx-yy+2ixy | m=-2 xx-yy-2ixy |
Oh | t2g xy,xz,yz | eg zz, xx-yy | |||
D3h | a1’ zz | e’ xx-yy, xy | e’’ xz, yz | ||
It is obvious that the <psi|m|psi>=m for |psi>= xy, xz, yz, zz, xx-yy. In other words, the orbital moments are quenched.