I'm reading Theorem 6.19 in textbook Real Analysis: Modern Techniques and Their Applications by Gerald B. Folland.
Suppose that $(X, \mathcal{M}, \mu)$ and $(Y, \mathcal{N}, \nu)$ are $\sigma$-finite measure spaces, and let $f$ be an $(\mathcal{M} \otimes \mathcal{N})$-measurable function on $X \times Y$.
a. If $f \geq 0$ and $1 \leq p<\infty$, then $$ \left[\int\left(\int f(x, y) d \nu(y)\right)^{p} d \mu(x)\right]^{1 / p} \leq \int\left[\int f(x, y)^{p} d \mu(x)\right]^{1 / p} d \nu(y) $$ b. If $1 \leq p \leq \infty, f(\cdot, y) \in L^{p}(\mu)$ for a.e. $y$, and the function $y \mapsto\|f(\cdot, y)\|_{p}$ is in $L^{1}(\nu)$, then $f(x, \cdot) \in L^{1}(\nu)$ for a.e. $x$, the function $x \mapsto \int f(x, y) d \nu(y)$ is in $L^{p}(\mu)$, and $$ \left\|\int f(\cdot, y) d \nu(y)\right\|_{p} \leq \int\|f(\cdot, y)\|_{p} d \nu(y). $$
In the proof of (b), he said that
Assertion (a) therefore follows from Theorem 6.14. When $p<\infty$, (b) follows from (a) (with $f$ replaced by $|f|$ ) and Fubini's theorem; when $p=\infty$, it is a simple consequence of the monotonicity of the integral.
Could you please explain?
Why do we need to use Fubini's theorem? I could not see the need of swapping differential operators here.
How is the monotonicity of the integral used to obtain the result for $p = \infty$ here?