Erwin Schrödinger

Schrödinger sin waagenliknang as det grünjlaag för kwantenmechaanisk bereegnangen:

${\displaystyle \mathrm {i} \hbar {\frac {\partial \psi }{\partial t}}=-{\frac {\hbar ^{2}}{2m}}\Delta \psi +V\psi }$ .