Abstract
The Schrödinger equation for a two-electron atomic system is reduced to an infinite system of linear equations. The linear operator defined by this system of equations is then shown to be compact in a region of the complex energy plane which excludes the various bound state and multiparticle scattering cuts (i.e., the eseential spectrum of the Hamiltonian of the two-electron atomic system). This permits one to truncate the infinite system of equations with the assurance that the N energy eigenvalues obtained from the N×N truncated system will uniformly approximate the lowest N energy eigenvalues of the original infinite system.
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