I) The proof for $L_1$ is simpler actually; here is an outline:
1) Prove that a linear map $f : E\to E'$ is continuous (even uniformly) iff it is continuous at zero (0); i.e.
$$\begin{align}
(\exists c\ \epsilon \ \mathbb{R}) \ |f(x)|\leq c|x|
\end{align}$$
2) Fourier transform is a linear functional defined on $L_1$. So, by (1) you only need to prove it is continuous at 0:
We have:
$$\begin{align}
F(f) = \int_{\mathbb{R}} f(x)e^{-j\omega x}dx
\end{align}$$
Where F is the Fourier operator defined on L1.
$$\begin{align}
|F(f)| = \left|\int_{\mathbb{R}} f(x)e^{-j\omega x}dx\right| \leq \int_{\mathbb{R}} |f(x)e^{-j\omega x}|dx \leq \int_{\mathbb{R}} |f(x)|dx = \left \| f \right \|_{L^1} < {\infty}
\end{align}$$
Thus
$$\begin{align}
\left | F(f) \right | \leq 1 \left \| f \right \|_{L^1},
\end{align}$$
This completes the proof (set c = 1)
II) Yes, you could use DCT, here's how:
Take any sequence $$x_n \to 0$$
Set $$ u_n(x) = f(x)e^{-i\omega (x\pm x_n)} \ \\ \ u(x) = f(x)e^{-i\omega x} $$
Clearly, $$ u_n \to u $$
Now, $$\ u\ is\ L^1,\ so\ is\ each\ u_n$$
We also have $$\left |u_n \right | \leq \left | f \right |\ and\ f\ is\ L^1$$
Now use DCT to get:
$$
\int_{\mathbb{R}}|u_n-u| \to 0\ as \ n \to \infty $$