Abstract
The factorized wavefunction approach to perturbation theory is applied to the spherical quadratic Zeeman problem in hydrogen. The ground and excited 2p states are considered. The results are in good agreement with other available results and provide a good upper bound to the complete Zeeman energy shifts. Transition strengths are calculated in good agreement with available results and the quantitative role of the residual non-spherical perturbation is briefly analyzed.
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