eiπ+1=0e^{i\pi} + 1 = 0
E=mc2E = mc^2
∇⋅E=ρε0\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon_0}
∫−∞∞e−x2 dx=π\int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}
iℏ∂∂t∣ψ⟩=H^∣ψ⟩i\hbar\frac{\partial}{\partial t}|\psi\rangle = \hat{H}|\psi\rangle
ζ(s)=∑n=1∞1ns\zeta(s) = \sum_{n=1}^{\infty} \frac{1}{n^s}
a2+b2=c2a^2 + b^2 = c^2
ΔxΔp≥ℏ2\Delta x \Delta p \geq \frac{\hbar}{2}
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