Spinor spherical harmonics

Not to be confused with Spin-weighted spherical harmonics.

In quantum mechanics, spin spherical harmonics Y_{l, s, j, m} are spinors eigenstates of the total angular momentum operator squared:

${\begin{aligned}\mathbf {j} ^{2}Y_{l,s,j,m}&=j(j+1)Y_{l,s,j,m}\\\mathrm {j} _{\mathrm {z} }Y_{l,s,j,m}&=mY_{l,s,j,m}\end{aligned}}$

where j = l + s. They are the natural spinorial analog of vector spherical harmonics.

For spin-1/2 systems, they are given in matrix form by

$Y_{j\pm {\frac {1}{2}},{\frac {1}{2}},j,m}={\frac {1}{\sqrt {2{\bigl (}j\pm {\frac {1}{2}}{\bigr )}+1}}}{\begin{pmatrix}\mp {\sqrt {j\pm {\frac {1}{2}}\mp m+{\frac {1}{2}}}}Y_{j\pm {\frac {1}{2}}}^{m-{\frac {1}{2}}}\\{\sqrt {j\pm {\frac {1}{2}}\pm m+{\frac {1}{2}}}}Y_{j\pm {\frac {1}{2}}}^{m+{\frac {1}{2}}}\end{pmatrix}}$

References

• Edmonds, A. R. (1957), Angular Momentum in Quantum Mechanics, Princeton University Press, ISBN 978-0-691-07912-7