The spinor spherical harmonics Yl, s, j, m are the spinors eigenstates of the total angular momentum operator squared:
where j = l + s, where j, l, and s are the (dimensionless) total, orbital and spin angular momentum operators, j is the total azimuthal quantum number and m is the total magnetic quantum number.
Under a parity operation, we have
For spin-1/2 systems, they are given in matrix form by789
where Y l m {\displaystyle Y_{l}^{m}} are the usual spherical harmonics.
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