You may continue by substituting the following results for a projectile into your expression
$$ x = v_0t\cos \theta $$
$$ R = \frac{v_0^2}{g}\sin2\theta $$
$$ h = v_0t\sin\theta - \frac{1}{2} g t^2 $$
and verify that
$$\frac{hR}{xR-x^2}= \tan\theta$$
The numerator is
$$hR = \left(x\tan\theta - \frac{gx^2}{2v_0^2\cos^2\theta}\right)\frac{v_0^2\sin 2\theta}{g}=x\tan\theta \left(\frac{v_0^2\sin 2\theta}{g}-x \right)$$
and the denominator
$$x(R-x) = x\left(\frac{v_0^2\sin 2\theta}{g}-x \right)$$
Their ratio comes out as
$$\frac{hR}{xR-x^2}= \tan\alpha + \tan\beta= \tan\theta$$