[step:Compute the sign and the function values under the decomposition]Fix $\sigma \in S_{p+q}$ and write $\sigma = \tau \circ (\pi \oplus \rho)$ with $\tau \in \operatorname{Sh}(p,q)$, $\pi \in S_p$, $\rho \in S_q$. Since $\operatorname{sgn}: S_{p+q} \to \{\pm 1\}$ is a group homomorphism, and the block-diagonal $\pi \oplus \rho$ has sign $\operatorname{sgn}(\pi) \operatorname{sgn}(\rho)$, we obtain
\begin{align*}
\operatorname{sgn}(\sigma) = \operatorname{sgn}(\tau)\, \operatorname{sgn}(\pi \oplus \rho) = \operatorname{sgn}(\tau)\, \operatorname{sgn}(\pi)\, \operatorname{sgn}(\rho).
\end{align*}
For the function values, observe that $\sigma(i) = \tau(\pi(i))$ for $1 \le i \le p$ and $\sigma(p+j) = \tau(p + \rho(j))$ for $1 \le j \le q$. Hence
\begin{align*}
\alpha(v_{\sigma(1)}, \dots, v_{\sigma(p)}) = \alpha(v_{\tau(\pi(1))}, \dots, v_{\tau(\pi(p))}).
\end{align*}
Because $\alpha \in \Lambda^p(V^*)$ is alternating, permuting its arguments by $\pi \in S_p$ produces a factor of $\operatorname{sgn}(\pi)$:
\begin{align*}
\alpha(v_{\tau(\pi(1))}, \dots, v_{\tau(\pi(p))}) = \operatorname{sgn}(\pi)\, \alpha(v_{\tau(1)}, \dots, v_{\tau(p)}).
\end{align*}
Similarly, since $\beta \in \Lambda^q(V^*)$ is alternating,
\begin{align*}
\beta(v_{\sigma(p+1)}, \dots, v_{\sigma(p+q)}) = \beta(v_{\tau(p+\rho(1))}, \dots, v_{\tau(p+\rho(q))}) = \operatorname{sgn}(\rho)\, \beta(v_{\tau(p+1)}, \dots, v_{\tau(p+q)}).
\end{align*}
Multiplying these three identities yields
\begin{align*}
&\operatorname{sgn}(\sigma)\, \alpha(v_{\sigma(1)}, \dots, v_{\sigma(p)})\, \beta(v_{\sigma(p+1)}, \dots, v_{\sigma(p+q)}) \\
&\qquad = \operatorname{sgn}(\tau)\, \operatorname{sgn}(\pi)\, \operatorname{sgn}(\rho)\, \cdot\, \operatorname{sgn}(\pi)\, \alpha(v_{\tau(1)}, \dots, v_{\tau(p)})\, \cdot\, \operatorname{sgn}(\rho)\, \beta(v_{\tau(p+1)}, \dots, v_{\tau(p+q)}) \\
&\qquad = \operatorname{sgn}(\tau)\, \alpha(v_{\tau(1)}, \dots, v_{\tau(p)})\, \beta(v_{\tau(p+1)}, \dots, v_{\tau(p+q)}),
\end{align*}
where the last equality uses $\operatorname{sgn}(\pi)^2 = \operatorname{sgn}(\rho)^2 = 1$.[/step]