Abstract
The osp(3‖2) superalgebra is realized, first by means of two supervectorial operators canonically conjugated, and then by differential operators acting on functions defined on E(3‖2). As for the vectorial representation of osp(1‖2) the eigenvalue problem yields to the superspherical harmonics.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have