For a two-electron ion of nuclear charge

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Atomic, Molecular & Optical Physics · Many-electron atoms and the periodic table

Deriving the Spectrum, Ch Helium: exchange and the variational method

Problem

For a two-electron ion of nuclear charge ZZ, the chapter gives the first-order energy E1=(−Z2+58Z)EhE_1 = \left(-Z^2 + \tfrac58Z\right)E_{\rm h} and the variational energy Evar=−(Z−516)2EhE_{\rm var} = -\left(Z-\tfrac{5}{16}\right)^2E_{\rm h}. Take Eh=27.211 eVE_{\rm h} = 27.211\,\mathrm{eV}. ((a)) Show that E1−EvarE_1 - E_{\rm var} is the same for every ZZ, and find it in eV. ((b)) The measured ground-state energies are −79.005 eV-79.005\,\mathrm{eV} for helium and −198.1 eV-198.1\,\mathrm{eV} for Li+\mathrm{Li}^+. For each, find how far EvarE_{\rm var} lies above the measured energy, in eV and as a percentage of the measured energy's size. ((c)) Use (a) and (b) to explain why the relative error of both estimates falls as ZZ grows.

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