8.11: Using Atomic Term Symbols to Describe Atomic Spectra
Around 1930 several spectroscopists using high resolution instruments found that lines in the hydrogen atom spectrum actually are not single lines but they are multiplets as shown for an isotopic mixture of hydrogen,\((H^1_{\alpha})\) and deuterium, (\(H^2_{\alpha}\)), in Figure \(\PageIndex{1}\). A multiplet consists of two or more closely spaced lines. Two lines together form a doublet, three a triplet, etc. Multiplets also are called fine structure. The term fine structure means the lines are spaced close together, i.e. finely spaced. Such fine structure also was found in spectra of oneelectron ions such as He+.
Figure \(\PageIndex{1}\): Photograph of the first line in the Balmer series for atomic hydrogen and deuterium. These lines are identified as \(H^1_{\alpha}\) (hydrogen) and \(H^2_{\alpha}\) (deuterium), respectively. From H.E. White, Introduction to Atomic Spectra (McGrawHill, New York, 1934) p. 132 and G.N. Lewis and F.H. Spedding, Phys. Rev. 43, 964 (1933). The doublet splitting for \(H^1_{\alpha}\) at 656.279 nm was measured to be 0.326 \(cm^{1}\).
You should recall that the \(H^1_{\alpha}\) line in the Balmer series at 656.279 nm was understood as resulting from a single transition of an electron from the n = 3 energy level to the n = 2 level. The observation of fine structure revealed that an orbital energy level diagram does not completely describe the energy levels of atoms. This fine structure also provided key evidence at the time for the existence of electron spin, which was used not only to give a qualitative explanation for the multiplets but also to furnish highly accurate calculations of the multiplet splittings.
SpinOrbit Couping
Specifying the orbital configuration of an atom does not uniquely identify the electronic state of the atom because the orbital angular momentum, the spin angular momentum, and the total angular momentum are not precisely specified. For example in the hydrogen 2p^{1} configuration, the electron can be in any of the three porbitals, \(m_l\) = +1, 0, and –1, and have spins with \(m_s\) = +1/2 or –1/2. Thus, there are 3 times 2 different possibilities or states. Also, the orbital and spin angular momentum of the electrons combine in multiple ways to produce angular momentum vectors that are characteristic of the entire atom not just individual electrons, and these different combinations can have different energies. This coupling of orbital and spin angular momentum occurs because both the electron spin and orbital motion produce magnetic dipole moments. As we have seen previously, the relationship between the angular momentum and the magnetic moment is given by the gyromagnetic ratio. These magnetic dipoles interact just like two tiny bar magnets attracting and repelling each other. This interaction is called spinorbit interaction. The interaction energy is proportional to the scalar product of the magnetic dipole moments, which are proportional to the angular momentum vectors.
\[E_{so} \propto S \cdot L \label{8.11.1}\]
with the following terms added to the Hamiltonian
\[\hat {H} _{so} \propto \hat {S} \cdot \hat {L} \label{8.11.2}\]
where the constant of proportionality is called the spinorbit coupling constant. The spinorbit interaction couples the spin motion and orbital motion of all the electrons together. This coupling means that exact wavefunctions are not eigenfunctions of the spin and orbital angular momentum operators separately. Rather the total angular momentum \(J = L+S\), the vector sum of the spin and orbital angular momentum, is required to be coupled for a completely accurate description of the system. Trying to describe the coupled system in terms of spin and orbital angular momentum separately is analogous to trying to describe the positions of two coupled bar magnets independently. It cannot be done; their interaction must be taken into account (Figure \(\PageIndex{1}\)).
Figure \(\PageIndex{1}\): An electron that orbits the nucleus induces a "current" and a magnetic field. Similarly, the rotating electron (really intrinsic spin) of the electron induces a different magnet. Both a magnetic (dipole) moments will interact with each other via spinorbit coupling to generate fine structure atomic spectra.Image used with permission (CCSA OpenStax).
Atomic Spectroscopy
Higher energy or excited orbital configurations also exist. The hydrogen atom can absorb energy, and the electron can be promoted to a higher energy orbital. The electronic states that result from these excited orbital configurations also are characterized or labeled by term symbols. The details of how to determine the term symbols for multielectron atoms and for cases where both the orbital and spin angular momentum differ from zero are given elsewhere, along with rules for determining the relative energies of the terms.
We have found that the selection rules for promoting a single electron moving from one atomic orbital to another via the absorption or emission of light are
\[ \Delta l = \pm 1 \label {8.11.6}\]
\[ \Delta m_l = 0, \pm 1 \label{8.11.7}\]
These selection rules arise from the conservation fo angular momentum during a spectroscopic transition and the fact that a photon has a spin 1. Within the limits of LS coupling, these rules can be expressed in terms of atomic term symbols resulting in the resulting RussellSaunders selection rules:
\[ \Delta S = 0 \label {8.11.8}\]
\[\Delta L = 0, \pm 1 \label {8.11.9}\]
\[\Delta J = 0, \pm 1,\label {8.11.10}\]
but \(J =0\) to \(J= 0\) is forbidden
\[\Delta m_J = 0, \pm 1 \label {8.11.11}\]
but \(m_J = 0\) to \(m_J = 0\) is forbidden if \(\Delta J = 0\). These selection rules result from the general properties of angular momentum such as the conservation of angular momentum and commutation relations. The \(\Delta L =0\) option in Equation \(\ref{8.11.9}\) does not violate the conservation of angular momentum discussed previously, since \(\Delta l = \pm 1\) is still required. The orbital angular momentum of an electron must change upon absorption, but this does not necessarily affect the overall momentum of the state given by Equation \(\ref{8.11.3}\).
The selection rules apply only to atoms that can be described with RussellSaunders (LS) coupling. These rules fail as the atomic number increases because the \(S\) and \(L\) quantum numbers become "bad" quantum numbers; this occurs when the jjcoupling coupling approach is more applicable. For example, the transition between single (\(S=1/2\) and triplet \(S=1\) states (volition of selection rule in Equation \(\ref{8.11.8}\)) are allowed and experimentally observed, in heavy atoms.
Example \(\PageIndex{1}\): Sodium Atoms
An example of this fine structure is the emission of sodium atoms.
There are six commonly observed lines in sodium lamps that are doublets are due to spinorbit coupling of L and S (Figure above does not show this splitting).
616.07 nm  615.42 nm  589.00 nm  589.59 nm  568.82 nm  568.26 nm 
How can these transitions be described in terms of transitions between microstates
Solution
We need to discussed states in terms of not only electron configurations, but in terms of microstates (i.e., term symbols) and the principal quantum number of the valence electron, \(n\):
 The ground state has a \((Ne]ns^1\) configuration, which has only one microstate \(^2S_{1/2}\)
 The excited state with the valence electron in the porbitals has an electron configuration of \([Ne]np^1\), which has two microstates: \(^2P_{3/2}\) and \(^2P_{1/2}\)
 The excited state with the valence electron in the porbitals has an electron configuration of \([Ne]nd^1\), which has two microstates of \(^2D_{5/2}\) and \(^2D_{3/2}\)
Observed lines can be explained:
 \(5S \rightarrow 3P\) gives two lines since the initial configuration has two microstates: 616.07, 615.42 nm
 \(3P \rightarrow 3S\) gives two lines since the terminal configuration has two microstates: 589.00, 589.59 nm
 \(4D \rightarrow 3P\) gives two lines since the terminal configuration has two microstates: 568.82, 568.26 nm
Splitting of the Sodium D Line
One notable atomic spectral line of sodium vapor is the socalled Dline, which may be observed directly as the sodium flametest line and also the major light output of low pressure sodium lamps (these produce pressure sodium lamps (these produce an unnatural yellow. The Dline is one of the classified Fraunhofer lines Sodium vapor in the upper layers of lines. Sodium vapor in the upper layers of the sun creates a dark line in the emitted spectrum of electromagnetic radiation by absorbing visible light in a band of wavelengths around 589.5 nm. This wavelength corresponds to transitions in atomic sodium in which the valenceelectron transitions from a 3s to 3p electronic state.
Closer examination of the visible spectrum of atomic sodium reveals that the Dline actually consists of two lines called the \(D_1\) and \(D_2\) lines at 589 6 nm and 589.0 nm, respectively. The splitting between these lines arises because of spinorbit coupling. Na has one unpaired electron (s = ½). If we consider the s > p transition, then for the excited state, p, we have \(L = 1\). Thus, \(j = 3/2\) or \(1/2\).
Now we want to apply these ideas to understand why multiplet structure is found in the luminescence spectrum of hydrogen and single electron ions. As we have said, the \(H_{\alpha}\) line in the Balmer series at 656.279 nm can be understood via a transition of an electron in a n = 3 atomic orbital to a n = 2 atomic orbital. When this spectral line was examined using highresolution instruments, it was found actually to be a doublet, i.e. two lines separated by 0.326 cm^{1}.
There are 9 degenerate orbitals associated with the n = 3 level, and 4 associated with the n = 2 level. Since an electron can be in any orbital with any one of two spins, we expect the total number of states to be twice the number of orbitals. The number of orbitals is given by \(n^2\) so there should be 8 states associated with n = 2 and 18 states associated with n = 3. Using the ideas of vector addition of angular momentum, the terms that result from having an electron in any one of these orbitals are given in Table \(\PageIndex{1}\).





\(^2S_{1/2}\) 


\(^2S_{1/2}\) 


\(^2P_{1/2}\), \(^2P_{3/2}\) 


\(^2S_{1/2}\) 


\(^2P_{1/2}\), \(^2P_{3/2}\) 


\(^2D_{3/2}\), \(^2D_{5/2}\) 

Table \(\PageIndex{1}\) shows that there are three terms associated with n = 2, and 5 terms associated with n = 3. In principle, each term can have a different energy. The degeneracy of each term is determined by the number of projections that the total angular momentum vector has on the zaxis. These projections depend on the \(m_J\) quantum number, which ranges from \(+J\) to \(–J\) in integer steps. J is the total angular momentum quantum number, which is given by the subscript in the term symbol. This relationship between \(m_J\) and J (\(m_J\) varies from \(+J\) to \(–J\) in integer steps) is true for any angular momentum vector.
Exercise \(\PageIndex{3}\)
Confirm that the nine term symbols in Table \(\PageIndex{1}\) are correct.
Exercise \(\PageIndex{4}\)
Confirm that the values for the degeneracy in Table \(\PageIndex{1}\) are correct and that the total number of states add up to 8 for n = 2 and 18 for n = 3.
The energies of the terms depend upon spinorbit coupling and relativistic corrections that need to be included in the Hamiltonian operator in order to provide a more complete description of the hydrogen atom. As a consequence of these effects, all terms with the same \(n\) and (J\) quantum numbers have the same energy, while terms with different values for \(n\) or \(J\) have different energies. The theoretical term splittings as given by H.E. White, Introduction to Atomic Spectra (McGrawHill, New York, 1934) pp. 132137 and are shown in Figure \(\PageIndex{2}\).
Figure \(\PageIndex{2}\): Energy level diagram for the electronic states of hydrogen corresponding to an electron with the principal quantum number n = 3 and n = 2. While the relative energies of the terms are drawn to scale, the energy of n = 3 relative to n = 2 is not. Transitions to the 2P_{3/2} and (2P_{1/2} and 2S_{1/2}) levels correspond to the two lines in the \(H^1_{\alpha}\) band, which have a measured separation of 0.326 cm^{1}.
Figure \(\PageIndex{2}\) shows 5 allowed transitions for the electron in the states associated with n = 3 to the states associated with n = 2. Of these five, two are most intense and are responsible for the doublet structure. These two transitions are indicated by the wide black lines at the bottom of the figure to correspond to the lines observed in the photographic spectrum shown in Figure \(\PageIndex{2}\). The other transitions contribute to the width of these lines or are not observed. The theoretical value for the doublet splitting is 0.328 cm^{1}, which is in excellent agreement with the measured value of 0.326 cm^{1}. The value of 0.328 cm^{1 }is obtained by taking the difference, 0.364 – 0.036 cm^{1},in the term splittings.
As we have just seen, the electronic states, as identified by the term symbols, are essential in understanding the spectra and energy level structure of atoms, but it also is important to associate the term symbols and states with the orbital electron configurations. The orbital configurations help us understand many of the general or coarse features of spectra and are necessary to produce a physical picture of how the electron density changes because of a spectroscopic transition.
Exercise \(\PageIndex{5}\)
Use the RussellSaunders selection rules to determine which transitions contribute to the \(H_{\alpha}\) line in the hydrogen spectrum.
Contributors
Adapted from "Quantum States of Atoms and Molecules" by David M. Hanson, Erica Harvey, Robert Sweeney, Theresa Julia Zielinski