The displacement equation is given by $Y(t) = A \sin(\omega t + \phi_0)$.
At $t=0$, the displacement is $Y(0) = A/2$.
Substituting into the equation: $A/2 = A \sin(0 + \phi_0) \implies \sin(\phi_0) = 1/2$.
This condition is satisfied for $\phi_0 = \frac{\pi}{6}$ and $\phi_0 = \frac{5\pi}{6}$ in the range $[0, 2\pi]$.
The velocity of the particle is given by the derivative of the displacement:
$v(t) = \frac{dY}{dt} = A\omega \cos(\omega t + \phi_0)$.
At $t=0$, the particle is moving in the negative direction, which means $v(0)<0$.
$v(0) = A\omega \cos(\phi_0)<0$.
Since A and $\omega$ are positive, this requires $\cos(\phi_0)<0$.
Now we check the two possible values for $\phi_0$:
If $\phi_0 = \frac{\pi}{6}$, then $\cos(\frac{\pi}{6}) = \frac{\sqrt{3}}{2}$, which is positive. This is not the correct phase.
If $\phi_0 = \frac{5\pi}{6}$, then $\cos(\frac{5\pi}{6}) = -\frac{\sqrt{3}}{2}$, which is negative. This matches the condition.
Therefore, the initial phase angle is $\phi_0 = \frac{5\pi}{6}$.