Consider two definite integrals:
\begin{equation} I_1 = \int_{R_1} f(x) \:dx\qquad I_2 = \int_{R_2} g(y) \:dy \end{equation}
Then, \begin{equation} I_1 \cdot I_2 = \left[ \int_{R_1} f(x) \:dx \right] \left[ \int_{R_2} g(y) \:dy\right] \end{equation}
Which under certain conditions becomes: \begin{equation} I_1 I_2 = \int_{R_1} \int_{R_2} f(x) g(y) \:dx \:dy \end{equation} I'm unsure whether I have to force the following, but here $f(x), g(y)$ are Real Valued Functions continuous on $R_1$ and $R_2$ respectively.
My question is: What theorem(s) is required in order for this property to hold? i.e. how do we know when we can combine and separate multiple integrals?