8. Zweielektronenatome

$\displaystyle \left[\vphantom{ -{\hbar^2 \over 2 \mu }\nabla_{r_1}^2 -{\hbar^2... ...ver 4 \pi \varepsilon_0 r_1} + {e^2 \over 4 \pi \varepsilon_0 r_{12}} }\right.$ - $\displaystyle {\hbar^2 \over 2 \mu}$ $\displaystyle \nabla_{r_1}^{2}$ - $\displaystyle {\hbar^2 \over 2 \mu}$ $\displaystyle \nabla_{r_1}^{2}$ - $\displaystyle {Z e^2 \over 4 \pi \varepsilon_0 r_1}$ - $\displaystyle {Z e^2 \over 4 \pi \varepsilon_0 r_1}$ + $\displaystyle {e^2 \over 4 \pi \varepsilon_0 r_{12}}$ $\displaystyle \left.\vphantom{ -{\hbar^2 \over 2 \mu }\nabla_{r_1}^2 -{\hbar^2... ...ver 4 \pi \varepsilon_0 r_1} + {e^2 \over 4 \pi \varepsilon_0 r_{12}} }\right]$ $\displaystyle \psi$ = E $\displaystyle \psi$

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