Building a many-body basis

Each single-particle state is labeled by the following quantum numbers:
  • Orbital angular momentum \( l \)
  • Intrinsic spin \( s \) = 1/2 for protons and neutrons
  • Angular momentum \( j = l \pm 1/2 \)
  • \( z \)-component \( j_z \) (or \( m \))
  • Some labeling of the radial wavefunction, typically \( n \) the number of nodes in the radial wavefunction, but in the case of harmonic oscillator one can also use the principal quantum number \( N \), where the harmonic oscillator energy is \( (N+3/2)\hbar \omega \).
In this format one labels states by \( n(l)_j \), with \( (l) \) replaced by a letter: \( s \) for \( l=0 \), \( p \) for \( l=1 \), \( d \) for \( l=2 \), \( f \) for \( l=3 \), and thenceforth alphabetical.