[step:Establish the bivariate normal orthant formula]We prove the auxiliary formula used twice below. Let $(U,V)$ be a centered bivariate normal random vector with $\mathbb{E}[U]=\mathbb{E}[V]=0$, $\operatorname{Var}(U)=\operatorname{Var}(V)=1$, and correlation $\rho \in [-1,1]$. Then
\begin{align*}
\mathbb{P}(U>0,\ V>0)=\frac14+\frac{1}{2\pi}\arcsin(\rho).
\end{align*}
For $|\rho|<1$, the joint density $f_\rho:\mathbb{R}^2\to[0,\infty)$ of $(U,V)$ with respect to $\mathcal{L}^2$ is
\begin{align*}
f_\rho(u,v)
=
\frac{1}{2\pi\sqrt{1-\rho^2}}
\exp\left(
-\frac{u^2-2\rho uv+v^2}{2(1-\rho^2)}
\right).
\end{align*}
Define $Q:(-1,1)\to[0,1]$ by
\begin{align*}
Q(\rho):=\int_0^\infty\int_0^\infty f_\rho(u,v)\,d\mathcal{L}^1(v)\,d\mathcal{L}^1(u).
\end{align*}
A direct differentiation of $f_\rho$ gives
\begin{align*}
\frac{\partial f_\rho}{\partial \rho}(u,v)
=
\frac{\partial^2 f_\rho}{\partial u\,\partial v}(u,v).
\end{align*}
Since $f_\rho$ and its first derivatives decay exponentially on every compact subinterval of $\rho\in(-1,1)$, differentiating under the integral sign and integrating by parts on $(0,\infty)^2$ are justified. Hence
\begin{align*}
Q'(\rho)
&=
\int_0^\infty\int_0^\infty
\frac{\partial^2 f_\rho}{\partial u\,\partial v}(u,v)
\,d\mathcal{L}^1(v)\,d\mathcal{L}^1(u)\\
&=
f_\rho(0,0)\\
&=
\frac{1}{2\pi\sqrt{1-\rho^2}}.
\end{align*}
At $\rho=0$, the variables $U$ and $V$ are independent standard normal variables, so
\begin{align*}
Q(0)=\mathbb{P}(U>0)\mathbb{P}(V>0)=\frac12\cdot\frac12=\frac14.
\end{align*}
Therefore, for $|\rho|<1$,
\begin{align*}
Q(\rho)
&=
Q(0)+\int_0^\rho Q'(s)\,d\mathcal{L}^1(s)\\
&=
\frac14+\int_0^\rho \frac{1}{2\pi\sqrt{1-s^2}}\,d\mathcal{L}^1(s)\\
&=
\frac14+\frac{1}{2\pi}\arcsin(\rho).
\end{align*}
For $\rho=1$, we have $V=U$ almost surely, hence $\mathbb{P}(U>0,V>0)=\mathbb{P}(U>0)=\frac12$. For $\rho=-1$, we have $V=-U$ almost surely, hence $\mathbb{P}(U>0,V>0)=0$. These agree with the same formula at $\rho=\pm1$.[/step]