The experimental values of log₁₀{T}1/2$(sec) plotted vs ${Z}d0.6/{Q}_{{{α}}}$ are shown to fall on a nearly universal straight line with ${log}₁₀T1/2(sec)=(9.54Zd0.6/ {}Q_α)-51.37, where Zd is the charge number of the daughter nucleus and Q_α is expressed in units of MeV. This behavior also numerically comes out of the semiclassical WKB calculation of the barrier penetration factor. The fine structure in the ratio of experiment over theory is briefly discussed.
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B. A. Brown (1992) studied this question.
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