Abstract
We present a numerical evaluation of the loop-after-loop contribution to the second-order self-energy for the ground state of hydrogenlike atoms with low nuclear charge numbers Z. The calculation is carried out in the Fried-Yennie gauge and without an expansion in $Z\ensuremath{\alpha}.$ Our calculation confirms the results of Mallampalli and Sapirstein and disagrees with the calculation by Goidenko and co-workers. A discrepancy between different calculations is investigated. An accurate fitting of the numerical results provides a detailed comparison with analytic calculations based on an expansion in the parameter $Z\ensuremath{\alpha}.$ We confirm the analytic results of order ${\ensuremath{\alpha}}^{2}(Z\ensuremath{\alpha}{)}^{5}$ but disagree with Karshenboim's calculation of the ${\ensuremath{\alpha}}^{2}(Z\ensuremath{\alpha}{)}^{6}{\mathrm{ln}}^{3}(Z\ensuremath{\alpha}{)}^{\ensuremath{-}2}$ contribution.
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