The magnetic dipole moment \( \mu \) of an electron moving in a circular orbit is given by:
\[
\mu = I \cdot A
\]
where \( I \) is the current due to the motion of the electron, and \( A \) is the area of the orbit.
For a revolving electron, the current \( I \) is given by the charge per unit time, which is:
\[
I = \frac{e}{T}
\]
where \( T \) is the time period of the electron’s revolution. The area \( A \) of the orbit is given by:
\[
A = \pi r^2
\]
where \( r \) is the radius of the orbit.
Now, the angular momentum \( L \) of the electron is given by:
\[
L = mvr
\]
where \( v \) is the velocity of the electron and \( r \) is the radius of the orbit.
Thus, the ratio between the magnetic dipole moment and angular momentum is:
\[
\frac{\mu}{L} = \frac{\frac{e}{T} \cdot \pi r^2}{mvr}
\]
We know that \( v = \frac{2\pi r}{T} \), so:
\[
\frac{\mu}{L} = \frac{\frac{e}{T} \cdot \pi r^2}{m \cdot \frac{2\pi r}{T} \cdot r} = \frac{e}{2m}
\]
Thus, the correct answer is option (C), \( \frac{e}{2m} \).