I encountered the following integral in a physical problem $$I=\int r^2 \text{J}_0(\alpha r) \text{I}_1(\beta r)\text{d}r$$ where $\text{J}_0$ is the Bessel function of first kind of order $0$ and $\text{I}_1$ is the modified Bessel function of order $1$. Also, $\alpha$ and $\beta$ are arbitrary real numbers.
It seems that MAPLE and WOLFRAM are not able to find the primitive. However, I think that there should be a tidy one in terms of Bessel functions.
My Thought
My instinct in integration tells me to use integration by parts and the recursive relations for Bessel functions. But I couldn't get any where yet.
First note that
$$ r\text{I}_1(\beta r)=\frac{\partial}{\partial\beta} \text{I}_0\left(\beta r\right).$$
Then we can write \begin{align} \mathcal{I}(t):=&\int_0^t r^2 \text{J}_0\left(\alpha r\right)\text{I}_1\left(\beta r\right) dr\\ =&\frac{\partial}{\partial\beta}\int_0^t r\text{J}_0\left(\alpha r\right)\text{I}_0\left(\beta r\right)dr\\ =& \frac{\partial}{\partial\beta}\left[\frac{t\left(\alpha \text{J}_1(\alpha t)\text{I}_0(\beta t)+\beta \text{J}_0(\alpha t)\text{I}_1(\beta t)\right)}{\alpha^2+\beta^2}\right]. \end{align} The last line follows from the formula 1.11.5.2 in Vol. II of Prudnikov-Brychkov-Marychev (and can of course be verified by direct differentiation).