J α ( x ) = ∑ m = 0 ∞ ( − 1 ...

${J}_{\alpha }\left(x\right)=\sum _{m=0}^{\mathrm{\infty }}\frac{\left(-1{\right)}^{m}}{m!\phantom{\rule{thinmathspace}{0ex}}\mathrm{\Gamma }\left(m+\alpha +1\right)}{\left(\frac{x}{2}\right)}^{2m+\alpha }$ $f\left(a\right)=\frac{1}{2\pi i}{\oint }_{\gamma }\frac{f\left(z\right)}{z-a}dz$ $\left[-\frac{{\hslash }^{2}}{2m}\frac{{\mathrm{\partial }}^{2}}{\mathrm{\partial }{x}^{2}}+V\right]\mathrm{\Psi }=i\hslash \frac{\mathrm{\partial }}{\mathrm{\partial }t}\mathrm{\Psi }$ ${a}^{2}+2ab+{b}^{2}={a}^{2}+{b}^{2}$ $x = \dfrac{-b \pm \sqrt{b^2-4ac}}{2a}$

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