152 Total Angular Momentum

An angular momentum equal to the sum of orbital and spin parts that is used to describe the full rotational properties of a quantum system.

\(\mathbf{J}=\mathbf{L}+\mathbf{S}\). The total angular momentum is the vector sum of orbital and spin angular momentum. This principle is used to couple \(\mathbf{L}\) and \(\mathbf{S}\) in atoms.

The total angular momentum is

\[ \mathbf{J} = \mathbf{L} + \mathbf{S} \]

where

  • \(\mathbf{J}\) is the total angular momentum.
  • \(\mathbf{L}\) is the orbital angular momentum.
  • \(\mathbf{S}\) is the spin angular momentum.

The \(\mathbf{J}\) algebra. The components of \(\mathbf{J}\) obey the same commutation relations as \(\mathbf{L}\). This principle is used to label states by \(j\) and \(m_{j}\).

The total-angular-momentum commutation relations are

\[ [J_{i}, J_{j}] = i\hbar\sum_{k}\epsilon_{ijk}J_{k} \]

where

  • \(J_{i}\) are the components of \(\mathbf{J}\).
  • \(\hbar\) is the reduced Planck constant.

The \(j=\ell\pm 1/2\) values. For one electron with orbital quantum number \(\ell\) and spin \(1/2\), the allowed \(j\) values are \(\ell\pm 1/2\). This principle is used to write fine-structure doublets.

The allowed \(j\) values are

\[ j = \ell \pm \dfrac{1}{2} \]

where

  • \(j\) labels eigenvalues of \(J^{2}\).
  • \(\ell\) is the orbital quantum number.

Conservation of \(\mathbf{J}\). In a rotationally invariant system, \(\mathbf{J}\) is often the conserved angular momentum. This principle is used to replace separate conservation of \(\mathbf{L}\) and \(\mathbf{S}\) when they are coupled.

Note: Also denoted \(\mathbf{J}\).

152.1 References

  1. Sakurai, J. J., & Napolitano, J. Modern Quantum Mechanics. Cambridge University Press, 2021. — \(\mathbf{J}=\mathbf{L}+\mathbf{S}\).
  2. Hall, B. C. Quantum Theory for Mathematicians. Springer, 2013. — \([J_{i},J_{j}]=i\hbar\sum_{k}\epsilon_{ijk}J_{k}\).
  3. Shankar, R. Fundamentals of Physics II. Yale University Press, 2020. — total angular momentum \(\mathbf{J}=\mathbf{L}+\mathbf{S}\).