Exact bound states for the central fraction power singular potential$V(r) = \alpha r^{2/3} + \beta r^{ - 2/3} + \gamma r^{ - 4/3}$.

Summary

We obtain here a set of exact bound-state solutions, out of infinite exact bound-state solutions, for the central fraction power singular potential$V(r) = \alpha r^{2/3} + \beta r^{ - 2/3} + \gamma r^{ - 4/3}$ by using a suitable ansatz. The bound-state solutions obtained here are normalizable and for each solution there is an interrelation between the parameters α, β, γ of the potential and the orbital angular-momentum quantum numberl.