I'm currently self-studying F. Cooper and al.'s Supersymmetry in Quantum Mechanics, and I need help working out a particular case on shape-invariance.
From a given superpotential of the form W(x)=ax3, where a>1, I can derive the two partner potentials:
V2,1=W(x)2±W(x)′=a2x6±3ax2
I can also say that V1(x) and V2(x) are shape-invariant potentials and write:
V2(x;a1)=V1(x;a2)+R(a1)
where a1 is a set of parameters, a2 is a function of a1 and R(a1) is independent of x.
From there, I am a bit lost. How do I work out the energy spectrum for the first few partner Hamiltonians?
This post imported from StackExchange Physics at 2014-10-23 21:54 (UTC), posted by SE-user Demosthene