b) In order to determine the energy and potential, we operate on the eigen-
The constant in the last term can be simplified to
In the limit the potential vanishes, and only the constant term in
the kinetic energy equals the eigenvalue. Thus, we find
c) To find the potential we subtract the kinetic energy from the eigenvalue
The potential has an attractive Coulomb term and a repulsive
term.
5.23 Algebra of Angular Momentum (Stony Brook)
a)
b) Since and commute, we will try to find eigenstates with eigenvalues
state with the kinetic energy operator. For this gives for the radial
part
and act on the eigenfunction:
of and denoted by where are real numbers:
QUANTUM MECHANICS 267