Step 1: Express radius of curvature in terms of kinetic energy.
For a charged particle moving perpendicular to a magnetic field, the radius is:
\[
r = \frac{mv}{qB}
\]
Step 2: Connect velocity to kinetic energy.
Kinetic energy $K = \frac{1}{2}mv^2$, so $v = \sqrt{\frac{2K}{m}}$. Substituting:
\[
r = \frac{m}{qB}\sqrt{\frac{2K}{m}} = \frac{\sqrt{2mK}}{qB}
\]
This shows that $r \propto \sqrt{K}$.
Step 3: Write the ratio of final to initial radius.
\[
\frac{r_f}{r_i} = \sqrt{\frac{K_f}{K_i}}
\]
Step 4: Use the given condition.
The particle loses half its kinetic energy, so $K_f = K_i / 2$:
\[
\frac{r_f}{r_i} = \sqrt{\frac{K_i/2}{K_i}} = \sqrt{\frac{1}{2}} = \frac{1}{\sqrt{2}}
\]
Step 5: Interpret the result.
The radius decreases by a factor of $1/\sqrt{2} \approx 0.707$. The particle curves more tightly in the magnetic field after losing energy.
Step 6: State the answer.
\[
\boxed{r_f = \frac{r_i}{\sqrt{2}}}
\]
The radius is reduced to $\dfrac{1}{\sqrt{2}}$ times the initial value.