Solution:
The electric potential \( V \) at the center of a charged half-ring is given by:
\[
V = \frac{1}{4\pi \epsilon_0} \int \frac{\lambda \, dl}{r}
\]
For a half-ring of radius \( r \), the total length is \( \pi r \), and the potential at the center is:
\[
V = \frac{\lambda}{4\pi \epsilon_0} \cdot \pi r \cdot \frac{1}{r} = \frac{\lambda}{4\epsilon_0}
\]
Thus, the electric potential at the center of the half-ring is:
\[
V = \frac{\lambda}{4 \epsilon_0}
\]
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