Step 1: Use speed at maximum height.
Let the initial speed of the projectile be
\[
u
\]
and the angle of projection be
\[
\theta.
\]
At maximum height, the vertical component of velocity becomes zero, so the speed at maximum height is only the horizontal component:
\[
u\cos\theta
\]
Given that this speed is half of the initial speed,
\[
u\cos\theta=\frac{u}{2}
\]
\[
\cos\theta=\frac{1}{2}
\]
Therefore,
\[
\theta=60^\circ
\]
Step 2: Write the formula for range.
The range of a projectile is
\[
R=\frac{u^2\sin 2\theta}{g}
\]
Substituting
\[
\theta=60^\circ,
\]
\[
R=\frac{u^2\sin 120^\circ}{g}
\]
Since
\[
\sin 120^\circ=\frac{\sqrt{3}}{2},
\]
we get
\[
R=\frac{\sqrt{3}u^2}{2g}
\]
Step 3: Write the formula for maximum height.
The maximum height is
\[
H=\frac{u^2\sin^2\theta}{2g}
\]
Substituting
\[
\theta=60^\circ,
\]
\[
H=\frac{u^2\sin^2 60^\circ}{2g}
\]
Since
\[
\sin 60^\circ=\frac{\sqrt{3}}{2},
\]
\[
\sin^2 60^\circ=\frac{3}{4}
\]
Therefore,
\[
H=\frac{u^2\cdot \frac{3}{4}}{2g}
\]
\[
H=\frac{3u^2}{8g}
\]
Step 4: Find the ratio \(\dfrac{R}{H}\).
\[
\frac{R}{H}
=
\frac{\frac{\sqrt{3}u^2}{2g}}{\frac{3u^2}{8g}}
\]
\[
=
\frac{\sqrt{3}u^2}{2g}\cdot \frac{8g}{3u^2}
\]
\[
=
\frac{4\sqrt{3}}{3}
\]
\[
=
\frac{4}{\sqrt{3}}
\]
Step 5: Final conclusion.
Therefore, the ratio between range and maximum height is
\[
\boxed{\frac{4}{\sqrt{3}}}
\]