The definition of the normalized Bessel functions is commonly understood to be: $$j_{\nu}(x)=\Gamma(\nu+1)\sum_{n=0}^{\infty}\frac{(-1)^{n}}{n!\Gamma(n+\nu+1)}(\frac{x}{2})^{2n}.$$
The question is why we have to choose $\nu>-\frac{1}{2}$.
The definition of the normalized Bessel functions is commonly understood to be: $$j_{\nu}(x)=\Gamma(\nu+1)\sum_{n=0}^{\infty}\frac{(-1)^{n}}{n!\Gamma(n+\nu+1)}(\frac{x}{2})^{2n}.$$
The question is why we have to choose $\nu>-\frac{1}{2}$.
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The Bessel function has asymptotics
$J_{\alpha}(x)\sim \frac{1}{\Gamma(1+\alpha)} (x/2)^{\alpha}$ for $x$ close to zero, my guess is for $L^2$ integrability, you need $\alpha>-1/2$.