A consequence of Yukawa's theory was a potential energy (in natural units), [frac{e^{-m r}}{r}] where (m) is

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A consequence of Yukawa's theory was a potential energy (in natural units),

\[\frac{e^{-m r}}{r}\]

where \(m\) is the mass of the mediating boson and \(r \approx 1.5 \mathrm{fm}\) is a measure of the range of the strong interaction. What value in \(\mathrm{MeV}\) is predicted for the mass of the boson?

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