Step 1: Understanding the relationship for magnification.
For a concave mirror, the magnification \( m \) is given by:
\[
m = \frac{-v}{u}
\]
Where:
- \( v \) is the image distance
- \( u \) is the object distance
- Given that the image is real, inverted, and doubly magnified, the magnification \( m = -2 \).
So, we have:
\[
-2 = \frac{-v}{18} \quad \Rightarrow \quad v = 36 \, \text{cm}
\]
Step 2: Using the mirror equation.
The mirror equation relates the object distance \( u \), image distance \( v \), and the focal length \( f \):
\[
\frac{1}{f} = \frac{1}{v} + \frac{1}{u}
\]
Since \( v = 36 \) cm and \( u = -18 \) cm (object is in front of the mirror), we substitute these values into the equation:
\[
\frac{1}{f} = \frac{1}{36} + \frac{1}{-18}
\]
\[
\frac{1}{f} = \frac{1}{36} - \frac{1}{18} = \frac{-1}{36}
\]
\[
f = -36 \, \text{cm}
\]
Step 3: Relating focal length to radius of curvature.
The radius of curvature \( R \) is related to the focal length \( f \) by:
\[
R = 2f
\]
So, the radius of curvature is:
\[
R = 2 \times (-36) = -72 \, \text{cm}
\]
Final Answer:
\[
\boxed{-72 \, \text{cm}}
\]