In particle, atomic and condensed matter physics, a Yukawa potential (also called a screened Coulomb potential) is a potential named after the Japanese physicist Hideki Yukawa. The potential is of the form: V Yukawa ( r ) = − g 2 e − α m r r , {\displaystyle V_{\text{Yukawa}}(r)=-g^{2}{\frac {e^{-\alpha mr}}{r}},} where g {\displaystyle g} is a magnitude scaling constant, i.e.
In particle, atomic and condensed matter physics, a Yukawa potential (also called a screened Coulomb potential) is a potential named after the Japanese physicist Hideki Yukawa. The potential is of the form: V Yukawa ( r ) = − g 2 e − α m r r , {\displaystyle V_{\text{Yukawa}}(r)=-g^{2}{\frac {e^{-\alpha mr}}{r}},} where g {\displaystyle g} is a magnitude scaling constant, i.e.
Source: Wikipedia "Yukawa potential" · CC BY-SA 4.0
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