Let $\left( V, W \right)$ be i.i.d standard normal, let $U$ be uniform on
$\left[ - \pi, \pi \right)$ independent of $R = \sqrt{V^2 + W^2}$ and let
$\varphi = \arcsin \rho$. Then the following vectors have the same
distributions (think about the Box-Muller transformation)
\begin{eqnarray*}
\left( X, Y \right) & \overset{d}{=} & \sqrt{2} \left( V \cos \varphi + W
\sin \varphi, W \right)\\
\left( V, W \right) & \overset{d}{=} & R \left( \cos U, \sin U \right)
\end{eqnarray*}
Implying
\begin{eqnarray*}
P \left[ X > 0, Y > 0 \right] & = & P \left[ \cos U \cos \varphi + \sin U
\sin \varphi > 0, \sin U > 0 \right]\\
& = & P \left[ U \in \left( \varphi - \frac{\pi}{2}, \varphi +
\frac{\pi}{2} \right) \cap \left( 0, \pi \right) \right]\\
& = & \frac{\varphi}{2 \pi} + \frac{1}{4}
\end{eqnarray*}
Here is an alternative proof:
Let $\phi$ be the density of the standard normal distribution
\begin{eqnarray*}
P \left[ X > 0, Y > 0 \right] & = & P \left[ X < 0, Y < 0 \right]\\
& = & \int_{- \infty}^0 \phi \left( z \right) \int_{- \infty}^0
\frac{1}{\sqrt{1 - \rho^2}} \phi \left( \frac{x - \rho z}{\sqrt{1 - \rho^2}}
\right) \mathrm{d} x \mathrm{d} z\\
& = & \int_{- \infty}^0 \phi \left( z \right) \int_{- \infty}^{- \frac{\rho
z}{\sqrt{1 - \rho^2}}} \phi \left( x \right) \mathrm{d} x \mathrm{d} z
\end{eqnarray*}
Let's call the above integral $h \left( \rho \right)$, then after some
simplifications
$$\frac{\partial h \left( \rho \right)}{\partial \rho} = \frac{1}{2 \pi
\sqrt{1 - \rho^2}} $$
By integrating back (or considering the problem as a first-order ordinary differential equation), $h \left( \rho \right) = \frac{1}{2 \pi} \arcsin \rho +
K$ where $K$ is some constant. By the special case of independence, $h \left( 0 \right) =
\frac{1}{4}$, you get the final solution
$$ P \left[ X > 0, Y > 0 \right] = \frac{1}{2 \pi} \arcsin \rho + \frac{1}{4}$$