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Fig. displays the oscillator strength per energy level and not per state. states are twofold degenerate due to the two possible l values, l 1, while states are nondegenerate as l 0. For this reason, when these states become nearly degenerate in the split-bubble regime, one transition has f ∼ 0.32 and the other f ∼ 0.65, a factor of 2 larger.
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