The shell of the three-dimensional isotropic oscillator holds states at one energy

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Symmetry, angular momentum and spin · Symmetry, angular momentum and spin

The Structure of Quantum Mechanics, Ch Symmetries, generators and conservation laws

Problem

The shell NN of the three-dimensional isotropic oscillator holds (N+1)(N+2)/2(N+1)(N+2)/2 states at one energy, and its orbital quantum numbers run l=N,N−2,…l=N,N-2,\dots down to 11 or 00. Take the shell N=4N=4. ((a)) List the values of ll in the shell and the dimension of the SO(3)SO(3) multiplet each one carries. Check that the dimensions add up to the shell's degeneracy. ((b)) Which states in the shell does rotational symmetry alone force to share one energy, and which coincidences does it leave unexplained? Is the l=0l=0 state forced to share its energy with any other state? ((c)) Add a small extra potential energy that depends only on rr but spoils the oscillator's special form. Which degeneracies in this shell does rotational symmetry still guarantee?

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