[guided]We now prove the marginal confidence statement for one contrast at a time. Define
\begin{align*}
c := t_{n-1;1-\alpha/(2k)} .
\end{align*}
For each $j \in \{1,\dots,k\}$, define the event
\begin{align*}
A_j
:=
\left\{
\omega \in \Omega :
|a_j^\top \bar X(\omega)-a_j^\top \mu|
\leq
c\sqrt{\frac{a_j^\top S(\omega)a_j}{n}}
\right\}.
\end{align*}
This is the event that the $j$th displayed interval contains its target value $a_j^\top \mu$.
There is a small degeneracy to handle first. If $a_j=0$, then the contrast is identically zero:
\begin{align*}
a_j^\top \bar X=0,
\qquad
a_j^\top \mu=0,
\qquad
a_j^\top S a_j=0.
\end{align*}
Hence the interval is $[0,0]$, which contains $0$ for every outcome $\omega \in \Omega$. Thus $A_j=\Omega$, and
\begin{align*}
\mathbb{P}(A_j^c)=0 \leq \frac{\alpha}{k}.
\end{align*}
Assume now that $a_j \neq 0$. Since $\Sigma$ is positive definite, the projected variance is strictly positive:
\begin{align*}
\sigma_j^2 := a_j^\top \Sigma a_j > 0.
\end{align*}
From the previous step, $Y_{1j},\dots,Y_{nj}$ are independent and identically distributed as $\mathcal{N}(a_j^\top \mu,\sigma_j^2)$. Therefore the usual studentized mean statistic
\begin{align*}
T_j
:=
\frac{\bar Y_j-a_j^\top \mu}{\sqrt{V_j/n}}
\end{align*}
has the Student $t$ distribution with $n-1$ degrees of freedom by the standard univariate normal theory result for the Student statistic (citing a result not yet in the wiki: Student $t$ statistic for a normal sample). The hypotheses of that result are satisfied here: the observations are independent, normally distributed, have common finite mean $a_j^\top \mu$, have common positive variance $\sigma_j^2$, and $n\geq 2$.
Because $\bar Y_j=a_j^\top \bar X$ and $V_j=a_j^\top S a_j$, the event $A_j$ can be rewritten as
\begin{align*}
A_j
=
\{|T_j|\leq c\}.
\end{align*}
The Student $t$ distribution is symmetric about $0$, and $c=t_{n-1;1-\alpha/(2k)}$ is chosen so that the upper tail probability is $\alpha/(2k)$. Hence the two tails together have probability $\alpha/k$:
\begin{align*}
\mathbb{P}(A_j^c)
=
\mathbb{P}(|T_j|>c)
=
\frac{\alpha}{2k}+\frac{\alpha}{2k}
=
\frac{\alpha}{k}.
\end{align*}
Combining this with the zero-contrast case gives, for every $j \in \{1,\dots,k\}$,
\begin{align*}
\mathbb{P}(A_j^c) \leq \frac{\alpha}{k}.
\end{align*}[/guided]