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Special Relativity ...

$$\beta = \frac{v}{c} \\ \gamma = \frac{1}{\sqrt{1 - \beta^2}} \\ ct' = \gamma ( ct - \beta x ) \\ x' = \gamma ( x - \beta ct ) \\ $$

... and Quantum Mechanics.

$$\frac{\hbar^2}{2m}\nabla^2\Psi + V(\mathbf{r})\Psi = -i\hbar \frac{\partial\Psi}{\partial t}$$

Yes, you get both in one fun-filled semester!