Abstract
In previous lectures, I have discussed how one can extract from QED an effective relativistic hamiltonian and shown how this can be expressed in terms of Slater integrals involving only radial functions defined in terms of a suitable one-body potential. From this point on, the process is very close to that employed in non-relativistic calculations of similar type.
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References
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© 1983 Plenum Press, New York
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Grant, I.P. (1983). Self-Consistency and Numerical Problems. In: Malli, G.L. (eds) Relativistic Effects in Atoms, Molecules, and Solids. NATO Advanced Science Institutes Series, vol 87. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-3596-2_5
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