[step:Use absolute continuity of Lebesgue integration to prove continuity of $F_X$]
For each $t\in\mathbb R$, the density property applied to $(-\infty,t]\in\mathcal B(\mathbb R)$ gives
\begin{align*}
F_X(t)=\int_{(-\infty,t]} f_X(u)\,d\mathcal L^1(u).
\end{align*}
[claim:Integrals of $L^1$ functions are small on sets of small measure]
Let $g:\mathbb R\to[0,\infty)$ be $\mathcal B(\mathbb R)$-measurable and satisfy
\begin{align*}
\int_{\mathbb R} g(u)\,d\mathcal L^1(u)<\infty.
\end{align*}
For every $\varepsilon>0$ there exists $\delta>0$ such that, whenever $E\in\mathcal B(\mathbb R)$ and $\mathcal L^1(E)<\delta$,
\begin{align*}
\int_E g(u)\,d\mathcal L^1(u)<\varepsilon.
\end{align*}
[/claim]
[proof]
Fix $\varepsilon>0$. For each $c>0$, define the Borel set
\begin{align*}
E_c:=\{u\in\mathbb R:g(u)>c\}.
\end{align*}
Let $\mathbb{1}_{E_c}:\mathbb R\to\{0,1\}$ denote the indicator function of $E_c$, defined by $\mathbb{1}_{E_c}(u)=1$ for $u\in E_c$ and $\mathbb{1}_{E_c}(u)=0$ for $u\notin E_c$. Define the [measurable function](/page/Measurable%20Function) $h_c:\mathbb R\to[0,\infty)$ by $h_c(u)=g(u)\mathbb{1}_{E_c}(u)$. If $(c_n)_{n=1}^{\infty}$ is any sequence in $(0,\infty)$ with $c_n\to\infty$, then $h_{c_n}(u)\to0$ for every $u\in\mathbb R$, and $0\le h_{c_n}\le g$. Since
\begin{align*}
\int_{\mathbb R} g(u)\,d\mathcal L^1(u)<\infty,
\end{align*}
the [dominated convergence theorem](/theorems/4), applied to the sequence $(h_{c_n})_{n=1}^{\infty}$ dominated by $g$, gives
\begin{align*}
\lim_{n\to\infty}\int_{E_{c_n}} g(u)\,d\mathcal L^1(u)=0.
\end{align*}
Because this holds for every sequence $c_n\to\infty$, we have
\begin{align*}
\lim_{c\to\infty}\int_{E_c} g(u)\,d\mathcal L^1(u)=0.
\end{align*}
Choose $c>0$ such that
\begin{align*}
\int_{\{u\in\mathbb R:g(u)>c\}} g(u)\,d\mathcal L^1(u)<\frac{\varepsilon}{2}.
\end{align*}
Define
\begin{align*}
\delta:=\frac{\varepsilon}{2c}.
\end{align*}
If $E\in\mathcal B(\mathbb R)$ and $\mathcal L^1(E)<\delta$, then split $E$ into $E\cap\{g\le c\}$ and $E\cap\{g>c\}$. By monotonicity of the [Lebesgue integral](/page/Lebesgue%20Integral),
\begin{align*}
\int_E g(u)\,d\mathcal L^1(u)\le c\,\mathcal L^1(E)+\int_{\{u\in\mathbb R:g(u)>c\}} g(u)\,d\mathcal L^1(u).
\end{align*}
Using the choices of $\delta$ and $c$ gives
\begin{align*}
\int_E g(u)\,d\mathcal L^1(u)<c\delta+\frac{\varepsilon}{2}=\varepsilon.
\end{align*}
[/proof]
Fix $t_0\in\mathbb R$ and $\varepsilon>0$. Taking $E=\mathbb R$ in the density identity gives
\begin{align*}
\int_{\mathbb R} f_X(u)\,d\mathcal L^1(u)=\mathbb P(X\in\mathbb R)=1,
\end{align*}
so $f_X$ satisfies the hypothesis of the claim. Apply the claim with $g=f_X$ to obtain $\delta>0$ such that every Borel set $E\subset\mathbb R$ with $\mathcal L^1(E)<\delta$ satisfies
\begin{align*}
\int_E f_X(u)\,d\mathcal L^1(u)<\varepsilon.
\end{align*}
If $t\in\mathbb R$ and $|t-t_0|<\delta$, then the symmetric difference of $(-\infty,t]$ and $(-\infty,t_0]$ is an interval of [Lebesgue measure](/page/Lebesgue%20Measure) $|t-t_0|$. Hence
\begin{align*}
|F_X(t)-F_X(t_0)|\le \int_{(\min\{t,t_0\},\max\{t,t_0\}]} f_X(u)\,d\mathcal L^1(u)<\varepsilon.
\end{align*}
Thus $F_X$ is continuous at $t_0$. Since $t_0$ was arbitrary, $F_X$ is continuous on $\mathbb R$.
[/step]