New applications of the Biedenharn-Temple operator

The Biedenharn approach to the Dirac-Coulomb problem is applied to a system considered by D’Hoker and Vinet, which consists of a spin $\text{2}$ particle in the combined field of a Dirac monopole plus a ${\lambda }^2\mathrm{/}{r}^2$ potential. The explicit solution is obtained by diagonalizing the Biedenharn-Temple operator, $\mathrm{\Gamma }$.