inline:$E = mc^2$
block
$$
i\hbar\frac{\partial \psi}{\partial t}
= \frac{-\hbar^2}{2m} \left(\frac{\partial^2}{\partial x^2} +
\frac{\partial^2}{\partial y^2} +
\frac{\partial^2}{\partial z^2} \right) \psi + V \psi$$
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inline:$E = mc^2$
block
$$
i\hbar\frac{\partial \psi}{\partial t}
= \frac{-\hbar^2}{2m} \left(\frac{\partial^2}{\partial x^2} +
\frac{\partial^2}{\partial y^2} +
\frac{\partial^2}{\partial z^2} \right) \psi + V \psi$$