Quantum Mechanics – Binding Energy vs. Ionization Energy of Hydrogen Explained

binding-energyhydrogenionization-energyquantum mechanics

Why is the binding energy of the electron in atomic hydrogen not the same as the ionization energy of hydrogen? The binding energy is $\approx 13.605874\text{ eV}$ (accounting for fine structure, see also the value in Griffiths'), and the ionization energy is $\approx 13.59844\text{ eV}$ NIST.
The ionization energy for molecular hydrogen is higher at $15.42593(5)\text{ eV}$ NIST.

The difference is about $0.00743\text{ eV}$, which is larger than the Lamb shift and hyperfine structure.

Is the ionization energy lower because it includes excited states of hydrogen? Or is the energy of a free electron lower when other atoms are present – the average radius increases with the principal quantum number, and it cannot increase without bound in the presence of other atoms.

Best Answer

You missed the reduced mass correction to the groundstate energy, which is bigger than the fine structure correction (and of course the Lamb shift). In other words, you missed the motion of the proton. Don't despair - you were right to think that the ionization energy should be very precisely measured and in exact agreement with ($-1$ times) the groundstate energy of hydrogen predicted by the schrodinger equation + fine structure + hyperfine structure + lamb shift + proton radius correction + further dirac equation corrections + higher order lamb shift etc.

I derive this result in more detail here (my most popular answer!). IIRC Griffiths doesn't cover this concept in the Hydrogen chapter because it requires discussion of the concept of a two-particle wavefunction, and it doesn't give rise to any interesting degeneracy splitting like fine structure does. Without fine strucure, the groundstate energy of hydrogen is (in SI units): $$ -\frac{\mu e^4}{2(4\pi\epsilon_0)^2\hbar^2} $$ Where $\mu$ is the reduced mass in the center of mass coordinates for the electron and the proton: $$ \mu=\frac{1}{\frac{1}{m_e}+\frac{1}{m_p}}\approx m_e\left(1-\frac{m_e}{m_p}\right) $$ Wolfram alpha gives me the value $13.5982873\text{ eV}$. The error is now well in line with fine structure corrections $O(\alpha^4m_ec^2=0.00015\text{ eV})$.

Finally, note that your mentioning of the molecular hydrogen binding energy is totally irrelevant - it's a completely different (and more complicated) quantum mechanical system, and the interaction between the two hydrogens gives a correction that is $O(1)$ (it cannot be thought of as a small correction to the hydrogen wavefunction).

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