# Solving the Schrödinger equation with potentials of all the fundamental forces.

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###### Where $$\dfrac{4}{3} \dfrac{\alpha_s(r) \hbar c}{r} + kr$$ is the potential for strong force,$$- \frac{g^2}{4 \pi c^2} \frac{e^{-mr}}{r}$$ is the Yukawa potential and $$-K\frac{1}{r}e^{-mr}$$ is the weak field potential.( The other two are the gravitational and Coulombic potentials).
asked Oct 15, 2016
recategorized Oct 15, 2016

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