[guided]The $t$-ratio construction closely parallels the proof of [t-Distribution of Normalised Coefficient Estimate](/theorems/1446): a standard normal over the square root of an independent $\chi^2_{n-p}/(n-p)$. The only new element is the extra independent noise term $\varepsilon^*$ in the numerator. We need to check carefully that this extra term does not disturb the independence between numerator and denominator.
*Summary of what needs to be independent.* The $t$-ratio $Z/\sqrt{W/(n-p)}$ requires $Z \perp\!\!\!\perp W$. Here $Z$ depends on both $\hat\beta$ (through $\hat Y^* = x^{*\top}\hat\beta$) and $\varepsilon^*$ (through $Y^* = x^{*\top}\beta + \varepsilon^*$), while $W = \mathrm{RSS}/\sigma^2$ depends on the training data through $\mathrm{RSS}$. So we must verify $\mathrm{RSS}$ is independent of $(\hat\beta, \varepsilon^*)$ jointly.
*Step 1: $\mathrm{RSS} \perp\!\!\!\perp \hat\beta$.* This is [Distributional Properties of the Normal Linear Model](/theorems/1445) part (3).
*Step 2: $\mathrm{RSS} \perp\!\!\!\perp \varepsilon^*$.* The new noise $\varepsilon^*$ is independent of $Y$ by hypothesis. Since $\mathrm{RSS}$ is a Borel-measurable function of $Y$ (explicitly $\mathrm{RSS} = Y^\top (I_n - P) Y$), and independence between $\varepsilon^*$ and $Y$ passes to $\mathrm{RSS} = \phi(Y)$ by $\sigma(\mathrm{RSS}) \subseteq \sigma(Y)$, we get $\mathrm{RSS} \perp\!\!\!\perp \varepsilon^*$.
*Step 3: Joint independence $\mathrm{RSS} \perp\!\!\!\perp (\hat\beta, \varepsilon^*)$.* This is strictly stronger than the two pairwise independences in Steps 1 and 2, but follows from them combined with the independence structure of the underlying data. The cleanest way is to check the joint distribution factorises.
The random vector $(Y, \varepsilon^*)$ has joint distribution $\mu_{Y} \otimes \mu_{\varepsilon^*}$ because $\varepsilon^* \perp\!\!\!\perp Y$. Applying the measurable map $(y, e) \mapsto (\mathrm{RSS}(y), \hat\beta(y), e)$, the image measure factors as the joint distribution of $(\mathrm{RSS}, \hat\beta)$ (which itself factors as $\mu_{\mathrm{RSS}} \otimes \mu_{\hat\beta}$ by [Distributional Properties of the Normal Linear Model](/theorems/1445) part (3)) times $\mu_{\varepsilon^*}$. So
\begin{align*}
\mu_{(\mathrm{RSS}, \hat\beta, \varepsilon^*)} = \mu_{\mathrm{RSS}} \otimes \mu_{\hat\beta} \otimes \mu_{\varepsilon^*},
\end{align*}
i.e., the three variables are mutually independent, and in particular $\mathrm{RSS}$ is independent of the pair $(\hat\beta, \varepsilon^*)$.
*Step 4: $W \perp\!\!\!\perp Z$.* Since $W = \mathrm{RSS}/\sigma^2$ is a measurable function of $\mathrm{RSS}$, and $Z$ is a measurable function of the pair $(\hat\beta, \varepsilon^*)$, the previous joint independence gives $W \perp\!\!\!\perp Z$ — measurable functions of independent variables remain independent.
*Why the extra $\varepsilon^*$ does not inflate the degrees of freedom.* This is the subtle point. One might worry that carrying around an extra normal in the numerator should "cost" us some chi-squared variability and reduce the degrees of freedom. It does not, because $\varepsilon^*$ is completely independent of the training data and therefore of $W$. The only degrees of freedom consumed in the denominator are the $p$ coefficients estimated from the $n$ training observations, leaving $n - p$ — exactly the $\chi^2_{n - p}$ degrees of freedom that appeared in the $t$-ratio for normalised coefficients.
Applying the definition of the $t$ distribution:
\begin{align*}
\frac{Z}{\sqrt{W/(n-p)}} \sim t_{n-p},
\end{align*}
and substituting the identity from Step 4,
\begin{align*}
\frac{\hat Y^* - Y^*}{\tilde\sigma \sqrt{\tau^2 + 1}} \sim t_{n-p}.
\end{align*}
This is the pivot used to construct prediction intervals for a future observation.[/guided]