Hund's rules

In atomic spectroscopy, Hund's rules predict the order of atomic energy levels with quantum numbers L, S and J. The rules are called after Friedrich Hund who formulated them in 1925.

LS coupling

A group of atomic energy levels, obtained by Russell-Saunders coupling, is concisely indicated by a term symbol. As discussed in the article Russell-Saunders coupling, closed shells and closed subshells have L = S = 0 and hence can be ignored in the coupling. A term (also known as multiplet) is a set of simultaneous eigenfunctions of L² (total orbital angular momentum squared) and S² (total spin angular momentum squared) with given quantum numbers L and S, respectively.

If there is no spin-orbit coupling, the functions of one term (fixed L and S) are degenerate (have the same energy). If there is weak spin-orbit coupling it is useful to diagonalize the matrix of the corresponding spin-orbit operator within the LS basis in the spirit of first-order perturbation theory. This introduces the new quantum number J, with |L-S| ≤ J ≤ L+S, that labels a 2(J+1)-dimensional energy level.

Level scheme of the carbon atom $\scriptstyle (1s)^{2}(2s)^{2}(2p)^{2}$. Drawing is not on scale. On the left the energy without any two-particle interaction. Then three-fold energy splitting after switching on electrostatic electron-electron interaction (L and S good quantum numbers). Then splittings after switching on first-order spin-orbit coupling (J good quantum number). Finally on the right Zeeman splittings in an external magnetic field.

Formulation of the rules

Hund's rules are:

1. Of the Russell-Saunders states arising from a given electron configuration those with the largest spin quantum number S lie lowest, those with the next largest next, and so on; in other words, the states with largest spin multiplicity are the most stable.
2. Of the group of terms with a given value of S, that with the largest value of L lies lowest.
3. Of the states with given values of S and L in an electronic configuration consisting of less than half the electrons in a closed subshell, the state with the smallest value of J is usually the most stable, and for a configuration consisting of more than half the electrons in a closed subshell the state with largest J is the most stable.

The levels of the second sort, largest J most stable, can be seen as arising from holes in a closed subshell.

Examples

• The ground state carbon atom, (1s)²(2s)²(2p)², gives by Russell-Saunders coupling a set of energy levels labeled by term symbols. Hund's rules predict the following order of the energies:

$^{3}P_{0}<^{3}P_{1}<^{3}P_{2}<^{1}D_{2}<^{1}S_{0}.$

• The ground state oxygen atom, (1s)²(2s)²(2p)⁴, (a two-hole state) gives by Russell-Saunders coupling a set of energy levels labeled by term symbols. Hund's rules predict the following order of the energies:

$^{3}P_{2}<^{3}P_{1}<^{3}P_{0}<^{1}D_{2}<^{1}S_{0}.$