ψ n ( x ) = 1 2 n n ! ⋅ ( α 2 π ) 1 / 4 ⋅ e − α 2 x 2 2 ⋅ H n ( α x ) , α = m ω ℏ {\displaystyle \psi _{n}(x)={\frac {1}{\sqrt {2^{n}\,n!}}}\cdot \left({\frac {\alpha ^{2}}{\pi }}\right)^{1/4}\cdot e^{-{\frac {\alpha ^{2}x^{2}}{2}}}\cdot H_{n}\left(\alpha x\right),\qquad \alpha ={\sqrt {\frac {m\omega }{\hbar }}}}
1 + 1 + 1 + 1 + 1 + ⋯ {\displaystyle {\sqrt {1+{\sqrt {1+{\sqrt {1+{\sqrt {1+{\sqrt {1+{\sqrt {\cdots }}}}}}}}}}}}}
D = E 4 π r 2 {\displaystyle D={\frac {E}{4\pi r^{2}}}}
