Prove that $\lim_{R\to 0}\int_R^\infty 2n_0 (\frac{r_0}{r})^{\alpha} \frac{r\mathrm{d}r}{\sqrt{r^2-R^2}}$ converges when $a<1$

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This problem is from Galaxies in the Universe: An Introduction, 2nd Edition

For the first question, it is solved here

But for the second question, it seems wierd that:

$$ \lim_{R\to 0}\Sigma(R) = \int_0^\infty 2n_0 (\frac{r_0}{r})^{\alpha} \mathrm{d}r = \int_0^b 2n_0 (\frac{r_0}{r})^{\alpha} \mathrm{d}r + \int_b^\infty 2n_0 (\frac{r_0}{r})^{\alpha} \mathrm{d}r $$

The first term is converged when $a<1$ but the second term is converged when $a>1$

Maybe I should not use the $\int_0^\infty 2n_0 (\frac{r_0}{r})^{\alpha} \mathrm{d}r$ and get back to:

$$ \lim_{R\to 0}\int_R^\infty 2n_0 (\frac{r_0}{r})^{\alpha} \frac{r\mathrm{d}r}{\sqrt{r^2-R^2}} $$